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Papers for Thursday, Mar 20 2025

Papers with local authors

Adam A. Miller, Natasha S. Abrams, Greg Aldering, Shreya Anand, Charlotte R. Angus, Iair Arcavi, Charles Baltay, Franz E. Bauer, Daniel Brethauer, Joshua S. Bloom, Hemanth Bommireddy, Marcio Catelan, Ryan Chornock, Peter Clark, Thomas E. Collett, Georgios Dimitriadis, Sara Faris, Francisco Forster, Anna Franckowiak, Christopher Frohmaier, Lluıs Galbany, Renato B. Galleguillos, Ariel Goobar, Claudia P. Gutierrez, Saarah Hall, Erica Hammerstein, Kenneth R. Herner, Isobel M. Hook, Macy J. Huston, Joel Johansson, Charles D. Kilpatrick, Alex G. Kim, Robert A. Knop, Marek P. Kowalski, Lindsey A. Kwok, Natalie LeBaron, Kenneth W. Lin, Chang Liu, Jessica R. Lu, Wenbin Lu, Ragnhild Lunnan, Kate Maguire, Lydia Makrygianni, Raffaella Margutti, Dan Maoz, Patrik Milan Veres, Thomas Moore, A. J. Nayana, Matt Nicholl, Jakob Nordin, Giuliano Pignata, Abigail Polin, Dovi Poznanski, Jose L. Prieto, David L. Rabinowitz, Nabeel Rehemtulla, Mickael Rigault, Dan Ryczanowski, Nikhil Sarin, Steve Schulze, Ved G. Shah, Xinyue Sheng, Samuel P. R. Shilling, Brooke D. Simmons, Avinash Singh, Graham P. Smith, Mathew Smith, Jesper Sollerman, Maayane T. Soumagnac, Christopher W. Stubbs, Mark Sullivan, Aswin Suresh, Benny Trakhtenbrot, Charlotte Ward, Eli Wiston, Helen Xiong, Yuhan Yao, Peter E. Nugent
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Paper 2 — arXiv:2503.14579
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Paper 2 — arXiv:2503.14579

We present the La Silla Schmidt Southern Survey (LS4), a new wide-field, time-domain survey to be conducted with the 1 m ESO Schmidt telescope. The 268 megapixel LS4 camera mosaics 32 2k$\times$4k fully depleted CCDs, providing a $\sim$20 deg$^2$ field of view with $1''$ pixel$^{-1}$ resolution. The LS4 camera will have excellent performance at longer wavelengths: in a standard 45 s exposure the expected 5$\sigma$ limiting magnitudes in $g$, $i$, $z$ are $\sim$21.5, $\sim$20.9, and $\sim$20.3 mag (AB), respectively. The telescope design requires a novel filter holder that fixes different bandpasses over each quadrant of the detector. Two quadrants will have $i$ band, while the other two will be $g$ and $z$ band and color information will be obtained by dithering targets across the different quadrants. The majority (90%) of the observing time will be used to conduct a public survey that monitors the extragalactic sky at both moderate (3 d) and high (1 d) cadence, as well as focused observations within the Galactic bulge and plane. Alerts from the public survey will be broadcast to the community via established alert brokers. LS4 will run concurrently with the Vera C. Rubin Observatory's Legacy Survey of Space and Time (LSST). The combination of LS4+LSST will enable detailed holistic monitoring of many nearby transients: high-cadence LS4 observations will resolve the initial rise and peak of the light curve while less-frequent but deeper observations by LSST will characterize the years before and after explosion. Here, we summarize the primary science objectives of LS4 including microlensing events in the Galaxy, extragalactic transients, the search for electromagnetic counterparts to multi-messenger events, and cosmology.

TaeHun Kim, Jinn-Ouk Gong, Donghui Jeong, Dong-Won Jung, Yeong Gyun Kim, Kang Young Lee
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Paper 3 — arXiv:2503.14581
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Paper 3 — arXiv:2503.14581

We demonstrate that primordial black holes (PBHs) lighter than $10^9 \, \text{g}$, which evaporated before the Big Bang nucleosynthesis, can induce significant isocurvature perturbations due to their biased clustering amplitude and the branching ratio of the Hawking radiation differing from the abundance ratio. By leveraging the upper bound on the isocurvature perturbations from the cosmic microwave background anisotropies reported by the Planck collaboration, we derive a new upper bound on the abundance of these light PBHs.

M. Abdul Karim, J. Aguilar, S. Ahlen, S. Alam, L. Allen, C. Allende Prieto, O. Alves, A. Anand, U. Andrade, E. Armengaud, A. Aviles, S. Bailey, C. Baltay, P. Bansal, A. Bault, J. Behera, S. BenZvi, D. Bianchi, C. Blake, S. Brieden, A. Brodzeller, D. Brooks, E. Buckley-Geer, E. Burtin, R. Calderon, R. Canning, A. Carnero Rosell, P. Carrilho, L. Casas, F. J. Castander, R. Cereskaite, M. Charles, E. Chaussidon, J. Chaves-Montero, D. Chebat, X. Chen, T. Claybaugh, S. Cole, A. P. Cooper, A. Cuceu, K. S. Dawson, A. de la Macorra, A. de Mattia, N. Deiosso, J. Della Costa, R. Demina, A. Dey, B. Dey, Z. Ding, P. Doel, J. Edelstein, D. J. Eisenstein, W. Elbers, P. Fagrelius, K. Fanning, E. Fernández-García, S. Ferraro, A. Font-Ribera, J. E. Forero-Romero, C. S. Frenk, C. Garcia-Quintero, L. H. Garrison, E. Gaztañaga, H. Gil-Marín, S. Gontcho A Gontcho, D. Gonzalez, A. X. Gonzalez-Morales, C. Gordon, D. Green, G. Gutierrez, J. Guy, B. Hadzhiyska, C. Hahn, S. He, M. Herbold, H. K. Herrera-Alcantar, M. Ho, K. Honscheid, C. Howlett, D. Huterer, M. Ishak, S. Juneau, N. V. Kamble, N. G. Karaçaylı, R. Kehoe, S. Kent, A. G. Kim, D. Kirkby, T. Kisner, S. E. Koposov, A. Kremin, A. Krolewski, O. Lahav, C. Lamman, M. Landriau, D. Lang, J. Lasker, J.M. Le Goff, L. Le Guillou

this https URL )

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Paper 22 — arXiv:2503.14738
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Paper 22 — arXiv:2503.14738

We present baryon acoustic oscillation (BAO) measurements from more than 14 million galaxies and quasars drawn from the Dark Energy Spectroscopic Instrument (DESI) Data Release 2 (DR2), based on three years of operation. For cosmology inference, these galaxy measurements are combined with DESI Lyman-$\alpha$ forest BAO results presented in a companion paper. The DR2 BAO results are consistent with DESI DR1 and SDSS, and their distance-redshift relationship matches those from recent compilations of supernovae (SNe) over the same redshift range. The results are well described by a flat $\Lambda$CDM model, but the parameters preferred by BAO are in mild, $2.3\sigma$ tension with those determined from the cosmic microwave background (CMB), although the DESI results are consistent with the acoustic angular scale $\theta_*$ that is well-measured by Planck. This tension is alleviated by dark energy with a time-evolving equation of state parametrized by $w_0$ and $w_a$, which provides a better fit to the data, with a favored solution in the quadrant with $w_0>-1$ and $w_a<0$. This solution is preferred over $\Lambda$CDM at $3.1\sigma$ for the combination of DESI BAO and CMB data. When also including SNe, the preference for a dynamical dark energy model over $\Lambda$CDM ranges from $2.8-4.2\sigma$ depending on which SNe sample is used. We present evidence from other data combinations which also favor the same behavior at high significance. From the combination of DESI and CMB we derive 95% upper limits on the sum of neutrino masses, finding $\sum m_\nu<0.064$ eV assuming $\Lambda$CDM and $\sum m_\nu<0.16$ eV in the $w_0w_a$ model. Unless there is an unknown systematic error associated with one or more datasets, it is clear that $\Lambda$CDM is being challenged by the combination of DESI BAO with other measurements and that dynamical dark energy offers a possible solution.

M. Abdul Karim, J. Aguilar, S. Ahlen, C. Allende Prieto, O. Alves, A. Anand, U. Andrade, E. Armengaud, A. Aviles, S. Bailey, A. Bault, S. BenZvi, D. Bianchi, C. Blake, A. Brodzeller, D. Brooks, E. Buckley-Geer, E. Burtin, R. Calderon, R. Canning, A. Carnero Rosell, P. Carrilho, L. Casas, F. J. Castander, R. Cereskaite, M. Charles, E. Chaussidon, J. Chaves-Montero, D. Chebat, T. Claybaugh, S. Cole, A. P. Cooper, A. Cuceu, K. S. Dawson, R. de Belsunce, A. de la Macorra, A. de Mattia, N. Deiosso, J. Della Costa, A. Dey, B. Dey, Z. Ding, P. Doel, J. Edelstein, D. J. Eisenstein, W. Elbers, P. Fagrelius, K. Fanning, S. Ferraro, A. Font-Ribera, J. E. Forero-Romero, C. Garcia-Quintero, L. H. Garrison, E. Gaztañaga, H. Gil-Marín, S. Gontcho A Gontcho, A. X. Gonzalez-Morales, C. Gordon, D. Green, G. Gutierrez, J. Guy, C. Hahn, M. Herbold, H. K. Herrera-Alcantar, M. Ho, K. Honscheid, C. Howlett, D. Huterer, M. Ishak, S. Juneau, N. G. Karaçaylı, R. Kehoe, S. Kent, D. Kirkby, T. Kisner, F.-S. Kitaura, S. E. Koposov, A. Kremin, O. Lahav, C. Lamman, M. Landriau, D. Lang, J. Lasker, J.M. Le Goff, L. Le Guillou, A. Leauthaud, M. E. Levi, Q. Li, T. S. Li, K. Lodha, M. Lokken, C. Magneville, M. Manera, P. Martini, W. Matthewson, P. McDonald, A. Meisner, J. Mena-Fernández, R. Miquel

this https URL )

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Paper 23 — arXiv:2503.14739
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Paper 23 — arXiv:2503.14739

We present the Baryon Acoustic Oscillation (BAO) measurements with the Lyman-alpha (LyA) forest from the second data release (DR2) of the Dark Energy Spectroscopic Instrument (DESI) survey. Our BAO measurements include both the auto-correlation of the LyA forest absorption observed in the spectra of high-redshift quasars and the cross-correlation of the absorption with the quasar positions. The total sample size is approximately a factor of two larger than the DR1 dataset, with forest measurements in over 820,000 quasar spectra and the positions of over 1.2 million quasars. We describe several significant improvements to our analysis in this paper, and two supporting papers describe improvements to the synthetic datasets that we use for validation and how we identify damped LyA absorbers. Our main result is that we have measured the BAO scale with a statistical precision of 1.1% along and 1.3% transverse to the line of sight, for a combined precision of 0.65% on the isotropic BAO scale at $z_{eff} = 2.33$. This excellent precision, combined with recent theoretical studies of the BAO shift due to nonlinear growth, motivated us to include a systematic error term in LyA BAO analysis for the first time. We measure the ratios $D_H(z_{eff})/r_d = 8.632 \pm 0.098 \pm 0.026$ and $D_M(z_{eff})/r_d = 38.99 \pm 0.52 \pm 0.12$, where $D_H = c/H(z)$ is the Hubble distance, $D_M$ is the transverse comoving distance, $r_d$ is the sound horizon at the drag epoch, and we quote both the statistical and the theoretical systematic uncertainty. The companion paper presents the BAO measurements at lower redshifts from the same dataset and the cosmological interpretation.

A. Brodzeller, M. Wolfson, D. M. Santos, M. Ho, T. Tan, M. M. Pieri, A. Cuceu, M. Abdul Karim, J. Aguilar, S. Ahlen, A. Anand, U. Andrade, E. Armengaud, A. Aviles, S. Bailey, A. Bault, D. Bianchi, D. Brooks, R. Canning, L. Casas, M. Charles, E. Chaussidon, J. Chaves-Montero, D. Chebat, T. Claybaugh, K. S. Dawson, R. de Belsunce, A. de la Macorra, A. de Mattia, Arjun Dey, Biprateep Dey, P. Doel, W. Elbers, S. Ferraro, A. Font-Ribera, J. E. Forero-Romero, C. Garcia-Quintero, L. H. Garrison, E. Gaztañaga, S. Gontcho A Gontcho, A. X. Gonzalez-Morales, D. Green, G. Gutierrez, J. Guy, C. Hahn, M. Herbold, H. K. Herrera-Alcantar, K. Honscheid, C. Howlett, D. Huterer, M. Ishak, S. Juneau, R. Kehoe, T. Kisner, A. Kremin, O. Lahav, C. Lamman, M. Landriau, J.M. Le Goff, L. Le Guillou, A. Leauthaud, M. E. Levi, Q. Li, M. Manera, P. Martini, A. Meisner, J. Mena-Fernandez, R. Miquel, J. Moustakas, A. Muñoz-Gutiérrez, A. D. Myers, S. Nadathur, L. Napolitano, H. E. Noriega, E. Paillas, N. Palanque-Delabrouille, W. J. Percival, C. Poppett, F. Prada, I. Pérez-Ràfols, C. Ramírez-Pérez, C. Ravoux, J. Rohlf, G. Rossi, E. Sanchez, D. Schlegel, M. Schubnell, F. Sinigaglia, D. Sprayberry, G. Tarlé, P. Taylor, W. Turner, M. Walther, B. A. Weaver, C. Yèche, R. Zhou, H. Zou, S. Zou

this https URL 21 pages, 13 figures, 3 tables

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Paper 24 — arXiv:2503.14740
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Paper 24 — arXiv:2503.14740

We present the Damped Ly$\alpha$ Toolkit for automated detection and characterization of Damped Ly$\alpha$ absorbers (DLA) in quasar spectra. Our method uses quasar spectral templates with and without absorption from intervening DLAs to reconstruct observed quasar forest regions. The best-fitting model determines whether a DLA is present while estimating the redshift and HI column density. With an optimized quality cut on detection significance ($\Delta \chi_{r}^2>0.03$), the technique achieves an estimated 72% purity and 71% completeness when evaluated on simulated spectra with S/N$>2$ that are free of broad absorption lines (BAL). We provide a catalog containing candidate DLAs from the DLA Toolkit detected in DESI DR1 quasar spectra, of which 21,719 were found in S/N$>2$ spectra with predicted $\log_{10} (N_\texttt{HI}) > 20.3$ and detection significance $\Delta \chi_{r}^2 >0.03$. We compare the Damped Ly$\alpha$ Toolkit to two alternative DLA finders based on a convolutional neural network (CNN) and Gaussian process (GP) models. We present a strategy for combining these three techniques to produce a high-fidelity DLA catalog from DESI DR2 for the Ly$\alpha$ forest baryon acoustic oscillation measurement. The combined catalog contains 41,152 candidate DLAs with $\log_{10} (N_\texttt{HI}) > 20.3$ from quasar spectra with S/N$>2$. We estimate this sample to be approximately 76% pure and 71% complete when BAL quasars are excluded.

U. Andrade, E. Paillas, J. Mena-Fernández, Q. Li, A. J. Ross, S. Nadathur, M. Rashkovetskyi, A. Pérez-Fernández, H. Seo, N. Sanders, O. Alves, X. Chen, N. Deiosso, M. Abdul Karim, S. Ahlen, E. Armengaud, A. Aviles, D. Bianchi, S. Brieden, A. Brodzeller, D. Brooks, E. Burtin, R. Calderon, R. Canning, A. Carnero Rosell, L. Casas, F. J. Castander, M. Charles, E. Chaussidon, J. Chaves-Montero, T. Claybaugh, S. Cole, A. Cuceu, K. S. Dawson, A. de la Macorra, A. de Mattia, J. Della Costa, A. Dey, B. Dey, Z. Ding, P. Doel, D. J. Eisenstein, W. Elbers, E. Fernández-García, S. Ferraro, A. Font-Ribera, J. E. Forero-Romero, C. Garcia-Quintero, L. H. Garrison, E. Gaztañaga, H. Gil-Marín, S. Gontcho A Gontcho, A. X. Gonzalez-Morales, C. Gordon, G. Gutierrez, J. Guy, C. Hahn, S. He, H. K. Herrera-Alcantar, K. Honscheid, C. Howlett, D. Huterer, M. Ishak, S. Juneau, R. Kehoe, D. Kirkby, T. Kisner, A. Kremin, O. Lahav, C. Lamman, M. Landriau, L. Le Guillou, A. Leauthaud, M. E. Levi, C. Magneville, M. Manera, P. Martini, W. Matthewson, A. Meisner, R. Miquel, J. Moustakas, A. Muñoz-Gutiérrez, D. Muñoz-Santos, A. D. Myers, L. Napolitano, J. A. Newman, H. E. Noriega, N. Palanque-Delabrouille, J. Pan, W. J. Percival, I. Pérez-Ràfols, C. Poppett, F. Prada, A. Raichoor, C. Ramírez-Pérez, C. Ravoux, G. Rossi, R. Ruggeri, L. Samushia

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Paper 26 — arXiv:2503.14742
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Paper 26 — arXiv:2503.14742

The Dark Energy Spectroscopic Instrument (DESI) data release 2 (DR2) galaxy and quasar clustering data represents a significant expansion of data from DR1, providing improved statistical precision in BAO constraints across multiple tracers, including bright galaxies (BGS), luminous red galaxies (LRGs), emission line galaxies (ELGs), and quasars (QSOs). In this paper, we validate the BAO analysis of DR2. We present the results of robustness tests on the blinded DR2 data and, after unblinding, consistency checks on the unblinded DR2 data. All results are compared to those obtained from a suite of mock catalogs that replicate the selection and clustering properties of the DR2 sample. We confirm the consistency of DR2 BAO measurements with DR1 while achieving a reduction in statistical uncertainties due to the increased survey volume and completeness. We assess the impact of analysis choices, including different data vectors (correlation function vs. power spectrum), modeling approaches and systematics treatments, and an assumption of the Gaussian likelihood, finding that our BAO constraints are stable across these variations and assumptions with a few minor refinements to the baseline setup of the DR1 BAO analysis. We summarize a series of pre-unblinding tests that confirmed the readiness of our analysis pipeline, the final systematic errors, and the DR2 BAO analysis baseline. The successful completion of these tests led to the unblinding of the DR2 BAO measurements, ultimately leading to the DESI DR2 cosmological analysis, with their implications for the expansion history of the Universe and the nature of dark energy presented in the DESI key paper.

K. Lodha, R. Calderon, W. L. Matthewson, A. Shafieloo, M. Ishak, J. Pan, C. Garcia-Quintero, D. Huterer, G. Valogiannis, L. A. Ureña-López, N. V. Kamble, D. Parkinson, A. G. Kim, G. B. Zhao, J. L. Cervantes-Cota, J. Rohlf, F. Lozano-Rodríguez, J. O. Román-Herrera, M. Abdul Karim, J. Aguilar, S. Ahlen, O. Alves, U. Andrade, E. Armengaud, A. Aviles, S. BenZvi, D. Bianchi, A. Brodzeller, D. Brooks, E. Burtin, R. Canning, A. Carnero Rosell, L. Casas, F. J. Castander, M. Charles, E. Chaussidon, J. Chaves-Montero, D. Chebat, T. Claybaugh, S. Cole, A. Cuceu, K. S. Dawson, A. de la Macorra, A. de Mattia, N. Deiosso, R. Demina, Arjun Dey, Biprateep Dey, Z. Ding, P. Doel, D. J. Eisenstein, W. Elbers, S. Ferraro, A. Font-Ribera, J. E. Forero-Romero, Lehman H. Garrison, E. Gaztañaga, H. Gil-Marín, S. Gontcho A Gontcho, A. X. Gonzalez-Morales, G. Gutierrez, J. Guy, C. Hahn, M. Herbold, H. K. Herrera-Alcantar, K. Honscheid, C. Howlett, S. Juneau, R. Kehoe, D. Kirkby, T. Kisner, A. Kremin, O. Lahav, C. Lamman, M. Landriau, L. Le Guillou, A. Leauthaud, M. E. Levi, Q. Li, C. Magneville, M. Manera, P. Martini, A. Meisner, J. Mena-Fernández, R. Miquel, J. Moustakas, D. Muñoz Santos, A. Muñoz-Gutiérrez, A. D. Myers, S. Nadathur, G. Niz, H. E. Noriega, E. Paillas, N. Palanque-Delabrouille, W. J. Percival, Matthew M. Pieri, C. Poppett, F. Prada, A. Pérez-Fernández

this https URL )

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Paper 27 — arXiv:2503.14743
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Paper 27 — arXiv:2503.14743

We conduct an extended analysis of dark energy constraints, in support of the findings of the DESI DR2 cosmology key paper, including DESI data, Planck CMB observations, and three different supernova compilations. Using a broad range of parametric and non-parametric methods, we explore the dark energy phenomenology and find consistent trends across all approaches, in good agreement with the $w_0w_a$CDM key paper results. Even with the additional flexibility introduced by non-parametric approaches, such as binning and Gaussian Processes, we find that extending $\Lambda$CDM to include a two-parameter $w(z)$ is sufficient to capture the trends present in the data. Finally, we examine three dark energy classes with distinct dynamics, including quintessence scenarios satisfying $w \geq -1$, to explore what underlying physics can explain such deviations. The current data indicate a clear preference for models that feature a phantom crossing; although alternatives lacking this feature are disfavored, they cannot yet be ruled out. Our analysis confirms that the evidence for dynamical dark energy, particularly at low redshift ($z \lesssim 0.3$), is robust and stable under different modeling choices.

L. Quilley, I. Damjanov, V. de Lapparent, A. Paulino-Afonso, H. Domínguez Sánchez, A. Ferré-Mateu, M. Huertas-Company, M. Kümmel, D. Delley, C. Spiniello, M. Baes, L. Wang, U. Kuchner, F. Tarsitano, R. Ragusa, M. Siudek, C. Tortora, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, P. Battaglia, R. Bender, A. Biviano, A. Bonchi, D. Bonino, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, F. J. Castander, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, A. Costille, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, C. A. J. Duncan, X. Dupac, S. Dusini, S. Escoffier, M. Fabricius, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, P. Fosalba, S. Fotopoulou, M. Frailis, E. Franceschi, S. Galeotta, K. George, B. Gillis, C. Giocoli, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, S. V. H. Haugan, H. Hoekstra, W. Holmes, I. M. Hook, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, B. Joachimi, E. Keihänen, S. Kermiche, A. Kiessling, B. Kubik, M. Kunz, H. Kurki-Suonio
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Paper 62 — arXiv:2503.15309
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Paper 62 — arXiv:2503.15309

We present the results of the single-component Sérsic profile fitting for the magnitude-limited sample of \IE$<23$ galaxies within the 63.1 deg$^2$ area of the Euclid Quick Data Release (Q1). The associated morphological catalogue includes two sets of structural parameters fitted using \texttt{SourceXtractor++}: one for VIS \IE images and one for a combination of three NISP images in \YE, \JE and \HE bands. We compare the resulting Sérsic parameters to other morphological measurements provided in the Q1 data release, and to the equivalent parameters based on higher-resolution \HST imaging. These comparisons confirm the consistency and the reliability of the fits to Q1 data. Our analysis of colour gradients shows that NISP profiles have systematically smaller effective radii ($R_{\rm e}$) and larger Sérsic indices ($n$) than in VIS. In addition, we highlight trends in NISP-to-VIS parameter ratios with both magnitude and $n_{\rm VIS}$. From the 2D bimodality of the $(u-r)$ colour-$\log(n)$ plane, we define a $(u-r)_{\rm lim}(n)$ that separates early- and late-type galaxies (ETGs and LTGs). We use the two subpopulations to examine the variations of $n$ across well-known scaling relations at $z<1$. ETGs display a steeper size--stellar mass relation than LTGs, indicating a difference in the main drivers of their mass assembly. Similarly, LTGs and ETGs occupy different parts of the stellar mass--star-formation rate plane, with ETGs at higher masses than LTGs, and further down below the Main Sequence of star-forming galaxies. This clear separation highlights the link known between the shutdown of star formation and morphological transformations in the Euclid imaging data set. In conclusion, our analysis demonstrates both the robustness of the Sérsic fits available in the Q1 morphological catalogue and the wealth of information they provide for studies of galaxy evolution with Euclid.

M. Huertas-Company, M. Walmsley, M. Siudek, P. Iglesias-Navarro, J. H. Knapen, S. Serjeant, H. J. Dickinson, L. Fortson, I. Garland, T. Géron, W. Keel, S. Kruk, C. J. Lintott, K. Mantha, K. Masters, D. O'Ryan, J. J. Popp, H. Roberts, C. Scarlata, J. S. Makechemu, B. Simmons, R. J. Smethurst, A. Spindler, M. Baes, E. M. Corsini, H. Domínguez Sánchez, E. Duran-Camacho, H. Fu, J. Junais, J. Mendez-Abreu, A. Nersesian, F. Shankar, M. N. Le, J. Vega-Ferrero, L. Wang, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, A. Basset, P. Battaglia, F. Bernardeau, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, S. Dusini, A. Ealet, S. Escoffier, M. Fabricius, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, S. Fotopoulou, M. Frailis, S. Galeotta, K. George, W. Gillard, B. Gillis, C. Giocoli, J. Gracia-Carpio, A. Grazian, F. Grupp, S. Gwyn
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Paper 64 — arXiv:2503.15311
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Paper 64 — arXiv:2503.15311

Stellar bars are key structures in disc galaxies, driving angular momentum redistribution and influencing processes such as bulge growth and star formation. Quantifying the bar fraction as a function of redshift and stellar mass is therefore important for constraining the physical processes that drive disc formation and evolution across the history of the Universe. Leveraging the unprecedented resolution and survey area of the Euclid Q1 data release combined with the Zoobot deep-learning model trained on citizen-science labels, we identify 7711 barred galaxies with $M_* \gtrsim 10^{10}M_\odot$ in a magnitude-selected sample $I_E < 20.5$ spanning $63.1 deg^2$. We measure a mean bar fraction of $0.2-0.4$, consistent with prior studies. At fixed redshift, massive galaxies exhibit higher bar fractions, while lower-mass systems show a steeper decline with redshift, suggesting earlier disc assembly in massive galaxies. Comparisons with cosmological simulations (e.g., TNG50, Auriga) reveal a broadly consistent bar fraction, but highlight overpredictions for high-mass systems, pointing to potential over-efficiency in central stellar mass build-up in simulations. These findings demonstrate Euclid's transformative potential for galaxy morphology studies and underscore the importance of refining theoretical models to better reproduce observed trends. Future work will explore finer mass bins, environmental correlations, and additional morphological indicators.

M. Siudek, M. Huertas-Company, M. Smith, G. Martinez-Solaeche, F. Lanusse, S. Ho, E. Angeloudi, P. A. C. Cunha, H. Domínguez Sánchez, M. Dunn, Y. Fu, P. Iglesias-Navarro, J. Junais, J. H. Knapen, B. Laloux, M. Mezcua, W. Roster, G. Stevens, J. Vega-Ferrero, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, S. Bardelli, P. Battaglia, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, F. J. Castander, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, J. Dinis, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, S. Dusini, S. Escoffier, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, S. Fotopoulou, M. Frailis, E. Franceschi, S. Galeotta, K. George, B. Gillis, C. Giocoli, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, S. Gwyn, S. V. H. Haugan, W. Holmes, I. M. Hook, F. Hormuth, A. Hornstrup, K. Jahnke, M. Jhabvala, E. Keihänen, S. Kermiche, A. Kiessling, B. Kubik, M. Kümmel, M. Kunz, H. Kurki-Suonio, Q. Le Boulc'h, A. M. C. Le Brun
0 votes
Paper 65 — arXiv:2503.15312
0 votes
Paper 65 — arXiv:2503.15312

Modern astronomical surveys, such as the Euclid mission, produce high-dimensional, multi-modal data sets that include imaging and spectroscopic information for millions of galaxies. These data serve as an ideal benchmark for large, pre-trained multi-modal models, which can leverage vast amounts of unlabelled data. In this work, we present the first exploration of Euclid data with AstroPT, an autoregressive multi-modal foundation model trained on approximately 300 000 optical and infrared Euclid images and spectral energy distributions (SEDs) from the first Euclid Quick Data Release. We compare self-supervised pre-training with baseline fully supervised training across several tasks: galaxy morphology classification; redshift estimation; similarity searches; and outlier detection. Our results show that: (a) AstroPT embeddings are highly informative, correlating with morphology and effectively isolating outliers; (b) including infrared data helps to isolate stars, but degrades the identification of edge-on galaxies, which are better captured by optical images; (c) simple fine-tuning of these embeddings for photometric redshift and stellar mass estimation outperforms a fully supervised approach, even when using only 1% of the training labels; and (d) incorporating SED data into AstroPT via a straightforward multi-modal token-chaining method improves photo-z predictions, and allow us to identify potentially more interesting anomalies (such as ringed or interacting galaxies) compared to a model pre-trained solely on imaging data.

C. Cleland, S. Mei, G. De Lucia, F. Fontanot, H. Fu, C. C. Lovell, M. Magliocchetti, N. Mai, D. Roberts, F. Shankar, J. G. Sorce, M. Baes, P. Corcho-Caballero, S. Eales, C. Tortora, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, P. Battaglia, A. Biviano, A. Bonchi, D. Bonino, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, F. J. Castander, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, X. Dupac, A. Ealet, S. Escoffier, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, S. Fotopoulou, M. Frailis, E. Franceschi, M. Fumana, S. Galeotta, K. George, B. Gillis, C. Giocoli, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, S. Gwyn, S. V. H. Haugan, J. Hoar, W. Holmes, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, B. Joachimi, E. Keihänen, S. Kermiche, A. Kiessling, B. Kubik, M. Kümmel, M. Kunz, H. Kurki-Suonio, O. Lahav, Q. Le Boulc'h, A. M. C. Le Brun, D. Le Mignant
0 votes
Paper 66 — arXiv:2503.15313
0 votes
Paper 66 — arXiv:2503.15313

The extent to which the environment affects galaxy evolution has been under scrutiny by researchers for decades. With the first data from Euclid, we can begin to study a wide range of environments and their effects as a function of redshift, using 63 sq deg of space-based data. In this paper, we present results from the Euclid Q1 Release, where we measure the passive-density and morphology-density relations at z=0.25--1. We determine if a galaxy is passive using the specific star-formation rate, and we classify the morphologies of galaxies using the Sérsic index n and the u-r colours. We measure the local environmental density of each galaxy using the Nth-nearest neighbour method. We find that at fixed stellar mass, the quenched fraction increases with increasing density up to z=0.75. This result shows the separability of the effects from the stellar mass and the environment, at least at z<0.75. At z>0.75, we observe weak environmental effects, with most high mass galaxies being quenched independently of environment. Up to z=0.75, the ETG fraction increases with density at fixed stellar mass, meaning the environment also transforms the morphology of the galaxy independently of stellar mass, at low mass. For high mass galaxies, almost all galaxies are early-types, with low impact from the environment. At z>0.75, the morphology depends mostly on stellar mass, with only low-mass galaxies being affected by the environment. Given that the morphology classifications use u-r colours, these are correlated to the star-formation rate, and as such our morphology results should be taken with caution; future morphology classifications should verify these results. To summarise, we identify the passive-density and morphology-density relations at z<0.75, but at z>0.75 the relations are less strong. At z>0.75, the uncertainties are large, and future Euclid data releases are key to confirm these trends.

A. Enia, L. Pozzetti, M. Bolzonella, L. Bisigello, W. G. Hartley, C. Saulder, E. Daddi, M. Siudek, G. Zamorani, P. Cassata, F. Gentile, L. Wang, G. Rodighiero, V. Allevato, P. Corcho-Caballero, H. Domínguez Sánchez, C. Tortora, M. Baes, Abdurro'uf, A. Nersesian, L. Spinoglio, J. Schaye, Y. Ascasibar, D. Scott, E. Duran-Camacho, S. Quai, M. Talia, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, A. Basset, P. Battaglia, R. Bender, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, F. J. Castander, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, S. Dusini, A. Ealet, S. Escoffier, M. Fabricius, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, S. Fotopoulou, M. Frailis, E. Franceschi, P. Franzetti, S. Galeotta, K. George, B. Gillis, C. Giocoli, P. Gómez-Alvarez, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, L. Guzzo, S. Gwyn, S. V. H. Haugan
0 votes
Paper 67 — arXiv:2503.15314
0 votes
Paper 67 — arXiv:2503.15314

The star-forming main sequence (SFMS) is a tight relation observed between stellar masses and star-formation rates (SFR) in a population of galaxies. The relation holds for different redshift, morphological, and environmental domains, and is a key to understanding the underlying relations between a galaxy budget of cold gas and its stellar content. \Euclid Quick Data Release 1 (Q1) gives the opportunity to investigate this fundamental relation in galaxy formation and evolution. We complement the \Euclid release with public IRAC observations of the \Euclid Deep Fields (EDFs), improving the quality of recovered photometric redshifts, stellar masses, and star-formation rates, as shown both from simulations and comparison with available spectroscopic redshifts. From Q1 data alone, we recover more than $\sim 30\,\mathrm{k}$ galaxies with $\log_{10}(M_\ast/M_\odot) > 11$, giving a precise constraint of the SFMS at the high-mass end. We investigated SFMS, in a redshift interval between $0.2$ and $3.0$, comparing our results with the existing literature and fitting them with a parameterisation taking into account the presence of a bending of the relation at the high-mass end, depending on the bending mass $M_0$. We find good agreement with previous results in terms of $M_0$ values. We also investigate the distribution of physical (e.g., dust absorption $A_V$ and formation age) and morphological properties (e.g., Sérsic index and radius) in the SFR--stellar mass plane, and their relation with the SFMS. These results highlight the potential of \Euclid in studying the fundamental scaling relations that regulate galaxy formation and evolution in anticipation of the forthcoming Data Release 1.

P. Corcho-Caballero, Y. Ascasibar, G. Verdoes Kleijn, C. C. Lovell, G. De Lucia, C. Cleland, F. Fontanot, C. Tortora, L. V. E. Koopmans, T. Moutard, C. Laigle, A. Nersesian, F. Shankar, N. Aghanim, B. Altieri, A. Amara, S. Andreon, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, P. Battaglia, A. Biviano, A. Bonchi, D. Bonino, E. Branchini, M. Brescia, J. Brinchmann, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, F. J. Castander, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, A. Costille, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, X. Dupac, A. Ealet, S. Escoffier, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, S. Fotopoulou, M. Frailis, E. Franceschi, M. Fumana, S. Galeotta, K. George, B. Gillis, C. Giocoli, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, L. Guzzo, S. Gwyn, S. V. H. Haugan, W. Holmes, I. M. Hook, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, E. Keihänen, S. Kermiche, A. Kiessling, B. Kubik, K. Kuijken, M. Kümmel, M. Kunz, H. Kurki-Suonio, Q. Le Boulc'h, A. M. C. Le Brun, D. Le Mignant, S. Ligori, P. B. Lilje, V. Lindholm
0 votes
Paper 68 — arXiv:2503.15315
0 votes
Paper 68 — arXiv:2503.15315

Investigating the drivers of the quenching of star formation in galaxies is key to understanding their evolution. The Euclid mission will provide rich spatial and spectral data from optical to infrared wavelengths for millions of galaxies, enabling precise measurements of their star formation histories. Using the first Euclid Quick Data Release (Q1), we developed a probabilistic classification framework, that combines the average specific star-formation rate ($\rm sSFR_\tau$) inferred over two timescales ($\tau={10^8,10^9}$ yr), to categorize galaxies as `Ageing' (secularly evolving), `Quenched' (recently halted star formation), or `Retired' (dominated by old stars). We validated this methodology using synthetic observations from the IllustrisTNG simulation. Two classification methods were employed: a probabilistic approach, integrating posterior distributions, and a model-driven method optimizing sample purity and completeness using IllustrisTNG. At $z<0.1$ and $M_\ast \gtrsim 3\times10^{8}\, M_\odot$, we obtain Euclid class fractions of 68-72%, 8-17%, and 14-19% for Ageing, Quenched, and Retired populations, respectively, consistent with previous studies. The evolution with redshift shows increasing/decreasing fraction of Ageing/Retired galaxies. The fraction of quenched systems shows a weaker dependence on stellar mass and redshift, varying between 5% and 15%. We analysed the mass-size-metallicity relation for each population. Ageing galaxies generally exhibit disc morphologies and low metallicities. Retired galaxies show compact structures and enhanced chemical enrichment, while Quenched galaxies form an intermediate population, more compact and chemically evolved than Ageing systems. This work demonstrates Euclid's great potential for elucidating the physical nature of the quenching mechanisms that govern galaxy evolution.

W. Roster, M. Salvato, J. Buchner, R. Shirley, E. Lusso, H. Landt, G. Zamorani, M. Siudek, B. Laloux, T. Matamoro Zatarain, F. Ricci, S. Fotopoulou, A. Ferré-Mateu, X. Lopez Lopez, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, P. Battaglia, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, S. Dusini, S. Escoffier, M. Fabricius, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, P. Fosalba, N. Fourmanoit, M. Frailis, E. Franceschi, S. Galeotta, K. George, B. Gillis, C. Giocoli, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, S. Gwyn, S. V. H. Haugan, W. Holmes, I. M. Hook, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, E. Keihänen, S. Kermiche, A. Kiessling, B. Kubik, M. Kümmel, M. Kunz, H. Kurki-Suonio, Q. Le Boulc'h, A. M. C. Le Brun, D. Le Mignant, S. Ligori, P. B. Lilje
0 votes
Paper 69 — arXiv:2503.15316
0 votes
Paper 69 — arXiv:2503.15316

To better understand the role of active galactic nuclei (AGN) in galaxy evolution, it is crucial to achieve a complete and pure AGN census. X-ray surveys are key to this, but identifying their counterparts (CTPs) at other wavelengths remains challenging due to their larger positional uncertainties and limited availability of deeper, uniform ancillary data. Euclid is revolutionising this effort, offering extensive coverage of nearly the entire extragalactic sky, particularly in the near-infrared bands, where AGN are more easily detected. With the first Euclid Quick Data Release (Q1), we identifyed, classifyed, and determined the redshifts of Euclid CTPs to known point-like sources from major X-ray surveys, including XMM-Newton, Chandra, and eROSITA. Using Bayesian statistics, combined with machine learning (ML), we identify the CTPs to 11 286 X-ray sources from the three X-ray telescopes. For the large majority of 10 194 sources, the associations are unique, with the remaining $\sim$ 10% of multi-CTP cases equally split between XMM-Newton and eROSITA. ML is then used to distinguish between Galactic (8%) and extragalactic (92%) sources. We computed photo-zs using deep learning for the 8617 sources detected in the 10th data release of the DESI Legacy Survey, reaching an accuracy and a fraction of outliers of about 5%. Based on their X-ray luminosities, over 99% of CTPs identified as extragalactic are classified as AGN, most of which appear unobscured given their hardness ratios. With this paper, we release our catalogue, which includes identifiers, basic X-ray properties, the details of the associations, and additional features such as Galactic/extragalactic classifications and photometric/spectroscopic redshifts. We also provide probabilities for sub-selecting the sample based on purity and completeness, allowing users to tailor the sample according to their specific needs.

A. La Marca, L. Wang, B. Margalef-Bentabol, L. Gabarra, Y. Toba, M. Mezcua, V. Rodriguez-Gomez, F. Ricci, S. Fotopoulou, T. Matamoro Zatarain, V. Allevato, F. La Franca, F. Shankar, L. Bisigello, G. Stevens, M. Siudek, W. Roster, M. Salvato, C. Tortora, L. Spinoglio, A. W. S. Man, J. H. Knapen, M. Baes, D. O'Ryan, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, S. Bardelli, P. Battaglia, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, A. Costille, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, A. Ealet, S. Escoffier, M. Fabricius, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, M. Frailis, E. Franceschi, S. Galeotta, K. George, B. Gillis, C. Giocoli, P. Gómez-Alvarez, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, L. Guzzo, S. Gwyn, S. V. H. Haugan, W. Holmes, I. M. Hook, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, B. Joachimi, E. Keihänen, S. Kermiche
0 votes
Paper 70 — arXiv:2503.15317
0 votes
Paper 70 — arXiv:2503.15317

Galaxy major mergers are a key pathway to trigger AGN. We present the first detection of major mergers in the Euclid Deep Fields and analyse their connection with AGN. We constructed a stellar-mass-complete ($M_*>10^{9.8}\,M_{\odot}$) sample of galaxies from the first quick data release (Q1), in the redshift range z=0.5-2. We selected AGN using X-ray data, optical spectroscopy, mid-infrared colours, and processing \IE observations with an image decomposition algorithm. We used CNNs trained on cosmological simulations to classify galaxies as mergers and non-mergers. We found a larger fraction of AGN in mergers compared to the non-merger controls for all AGN selections, with AGN excess factors ranging from 2 to 6. Likewise, a generally larger merger fraction ($f_{merg}$) is seen in active galaxies than in the non-active controls. We analysed $f_{merg}$ as a function of the AGN bolometric luminosity ($L_{bol}$) and the contribution of the point-source to the total galaxy light in the \IE-band ($f_{PSF}$) as a proxy for the relative AGN contribution fraction. We uncovered a rising $f_{merg}$, with increasing $f_{PSF}$ up to $f_{PSF}=0.55$, after which we observed a decreasing trend. We then derived the point-source luminosity ($L_{PSF}$) and showed that $f_{merg}$ monotonically increases as a function of $L_{PSF}$ at z<0.9, with $f_{merg}>$50% for $L_{PSF}>2\,10^{43}$ erg/s. At z>0.9, $f_{merg}$ rises as a function of $L_{PSF}$, though mergers do not dominate until $L_{PSF}=10^{45}$ erg/s. For X-ray and spectroscopic AGN, we computed $L_{bol}$, which has a positive correlation with $f_{merg}$ for X-ray AGN, while shows a less pronounced trend for spectroscopic AGN due to the smaller sample size. At $L_{bol}>10^{45}$ erg/s, AGN mostly reside in mergers. We concluded that mergers are strongly linked to the most powerful, dust-obscured AGN, associated with rapid supermassive black hole growth.

B. Margalef-Bentabol, L. Wang, A. La Marca, V. Rodriguez-Gomez, A. Humphrey, S. Fotopoulou, F. Ricci, Y. Toba, G. Stevens, M. Mezcua, W. Roster, J. H. Knapen, M. Salvato, M. Siudek, F. Shankar, T. Matamoro Zatarain, L. Spinoglio, P. Dayal, J. Petley, R. Kondapally, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, P. Battaglia, A. Biviano, A. Bonchi, D. Bonino, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, A. Costille, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, A. Ealet, S. Escoffier, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, M. Frailis, E. Franceschi, S. Galeotta, K. George, B. Gillis, C. Giocoli, P. Gómez-Alvarez, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, L. Guzzo, S. Gwyn, S. V. H. Haugan, W. Holmes, I. M. Hook, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, E. Keihänen, S. Kermiche, A. Kiessling, B. Kubik, M. Kümmel
0 votes
Paper 71 — arXiv:2503.15318
0 votes
Paper 71 — arXiv:2503.15318

Active galactic nuclei (AGN) play a key role in galaxy evolution but are challenging to identify due to their varied observational signatures. Furthermore, understanding their impact requires quantifying their strength relative to their host galaxies. We developed a deep learning (DL) model for identifying AGN in imaging data by deriving the contribution of the central point source. Trained on Euclidised mock galaxy images with injected AGN levels, in the form of varying contributions of the point-spread function (PSF), our model can precisely and accurately recover the injected AGN contribution fraction $f_{\rm PSF}$, with a mean difference between the predicted and true $f_{\rm PSF}$ of $-0.0078$ and an overall root mean square error (RMSE) of 0.051. This method moves beyond binary AGN classification, enabling precise AGN contribution measurements. Applying our model to a stellar-mass-limited sample ($M_{\ast} \ge 10^{9.8} M_{\odot}$, $0.5 \le z \le 2.0$) from the first \Euclid quick data release (Q1), we identify $48,840 \pm 78$ AGN over 63.1 deg$^2$ ($7.8\pm0.1$%) using a threshold of $f_{\rm PSF} > 0.2$. We compare our DL-selected AGN with those identified in X-ray, mid-infrared (MIR), and optical spectroscopy and investigate their overlapping fractions depending on different thresholds on the PSF contribution. We find that the overlap increases with increasing X-ray or bolometric AGN luminosity. The AGN luminosity in the $I_{\rm E}$ filter correlates with host galaxy stellar mass, suggesting faster supermassive black hole (SMBH) growth in more massive galaxies. Moreover, the mean relative contribution of the AGN is higher in quiescent galaxies than in star-forming ones. Starburst galaxies and the most massive galaxies (across the star-formation main sequence) tend to host the most luminous AGN, indicating concomitant assembly of the SMBH and the host galaxy.

F. Tarsitano, S. Fotopoulou, M. Banerji, J. Petley, A. L. Faisst, M. Tucci, S. Tacchella, Y. Toba, H. Landt, Y. Fu, P. A. C. Cunha, K. Duncan, W. Roster, M. Salvato, B. Laloux, P. Dayal, F. Ricci, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, P. Battaglia, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, A. Costille, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, S. Escoffier, M. Fabricius, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, M. Frailis, E. Franceschi, S. Galeotta, K. George, W. Gillard, B. Gillis, C. Giocoli, P. Gómez-Alvarez, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, L. Guzzo, S. Gwyn, S. V. H. Haugan, W. Holmes, I. M. Hook, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, E. Keihänen, S. Kermiche, A. Kiessling, B. Kubik, M. Kümmel, M. Kunz, H. Kurki-Suonio, Q. Le Boulc'h
0 votes
Paper 72 — arXiv:2503.15319
0 votes
Paper 72 — arXiv:2503.15319

Red quasars constitute an important but elusive phase in the evolution of supermassive black holes, where dust obscuration can significantly alter their observed properties. They have broad emission lines, like other quasars, but their optical continuum emission is significantly reddened, which is why they were traditionally identified based on near- and mid-infrared selection criteria. This work showcases the capability of the \Euclid space telescope to find a large sample of red quasars, using \Euclid near infrared (NIR) photometry. We first conduct a forecast analysis, comparing a synthetic catalogue of red QSOs with COSMOS2020. Using template fitting, we reconstruct \Euclid-like photometry for the COSMOS sources and identify a sample of candidates in a multidimensional colour-colour space achieving $98\%$ completeness for mock red QSOs with $30\%$ contaminants. To refine our selection function, we implement a probabilistic Random Forest classifier, and use UMAP visualisation to disentangle non-linear features in colour-space, reaching $98\%$ completeness and $88\%$ purity. A preliminary analysis of the candidates in the \Euclid Deep Field Fornax (EDF-F) shows that, compared to VISTA+DECAm-based colour selection criteria, \Euclid's superior depth, resolution and optical-to-NIR coverage improves the identification of the reddest, most obscured sources. Notably, the \Euclid exquisite resolution in the $I_E$ filter unveils the presence of a candidate dual quasar system, highlighting the potential for this mission to contribute to future studies on the population of dual AGN. The resulting catalogue of candidates, including more the 150 000 sources, provides a first census of red quasars in \Euclid Q1 and sets the groundwork for future studies in the Euclid Wide Survey (EWS), including spectral follow-up analyses and host morphology characterisation.

T. Matamoro Zatarain, S. Fotopoulou, F. Ricci, M. Bolzonella, F. La Franca, A. Viitanen, G. Zamorani, M. B. Taylor, M. Mezcua, B. Laloux, A. Bongiorno, K. Jahnke, G. Stevens, R. A. Shaw, L. Bisigello, W. Roster, Y. Fu, B. Margalef-Bentabol, A. La Marca, F. Tarsitano, A. Feltre, J. Calhau, X. Lopez Lopez, M. Scialpi, M. Salvato, V. Allevato, M. Siudek, C. Saulder, D. Vergani, M. N. Bremer, L. Wang, M. Giulietti, D. M. Alexander, D. Sluse, F. Shankar, L. Spinoglio, D. Scott, R. Shirley, H. Landt, M. Selwood, Y. Toba, P. Dayal, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, S. Bardelli, A. Basset, P. Battaglia, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, F. J. Castander, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, S. Dusini, A. Ealet, S. Escoffier, M. Fabricius, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, N. Fourmanoit, M. Frailis, E. Franceschi
0 votes
Paper 73 — arXiv:2503.15320
0 votes
Paper 73 — arXiv:2503.15320

We present a catalogue of candidate active galactic nuclei (AGN) in the $Euclid$ Quick Release (Q1) fields. For each $Euclid$ source we collect multi-wavelength photometry and spectroscopy information from Galaxy Evolution Explorer (GALEX), $Gaia$, Dark Energy Survey (DES), Wise-field Infrared Survey Explorer (WISE), $Spitzer$, Dark Energy Survey (DESI), and Sloan Digital Sky Survey (SDSS), including spectroscopic redshift from public compilations. We investigate the AGN contents of the Q1 fields by applying selection criteria using $Euclid$ colours and WISE-AllWISE cuts finding respectively 292,222 and 65,131 candidates. We also create a high-purity QSO catalogue based on $Gaia$ DR3 information containing 1971 candidates. Furthermore, we utilise the collected spectroscopic information from DESI to perform broad-line and narrow-line AGN selections, leading to a total of 4392 AGN candidates in the Q1 field. We investigate and refine the Q1 probabilistic random forest QSO population, selecting a total of 180,666 candidates. Additionally, we perform SED fitting on a subset of sources with available $z_{\text{spec}}$, and by utilizing the derived AGN fraction, we identify a total of 7766 AGN candidates. We discuss purity and completeness of the selections and define two new colour selection criteria ($JH$_$I_{\text{E}}Y$ and $I_{\text{E}}H$_$gz$) to improve on purity, finding 313,714 and 267,513 candidates respectively in the Q1 data. We find a total of 229,779 AGN candidates equivalent to an AGN surface density of 3641 deg$^{-2}$ for $18<I_{\text{E}}\leq 24.5$, and a subsample of 30,422 candidates corresponding to an AGN surface density of 482 deg$^{-2}$ when limiting the depth to $18<I_{\text{E}}\leq 22$. The surface density of AGN recovered from this work is in line with predictions based on the AGN X-ray luminosity functions.

G. Girardi, G. Rodighiero, L. Bisigello, A. Enia, A. Grazian, E. Dalla Bontà, E. Daddi, S. Serjeant, G. Gandolfi, C. C. Lovell, K. I. Caputi, A. Bianchetti, A. Vietri, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, P. Battaglia, R. Bender, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, S. Dusini, A. Ealet, S. Escoffier, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, S. Fotopoulou, M. Frailis, E. Franceschi, S. Galeotta, K. George, B. Gillis, C. Giocoli, P. Gómez-Alvarez, J. Gracia-Carpio, B. R. Granett, F. Grupp, S. Gwyn, S. V. H. Haugan, W. Holmes, I. M. Hook, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, E. Keihänen, S. Kermiche, A. Kiessling, B. Kubik, K. Kuijken, M. Kümmel, M. Kunz, H. Kurki-Suonio, Q. Le Boulc'h, A. M. C. Le Brun, D. Le Mignant, S. Ligori, P. B. Lilje
0 votes
Paper 75 — arXiv:2503.15322
0 votes
Paper 75 — arXiv:2503.15322

Our understanding of cosmic star-formation at $z>3$ used to largely rely on rest-frame UV observations. However, these observations overlook dusty and massive sources, resulting in an incomplete census of early star-forming galaxies. Recently, infrared data from Spitzer and the James Webb Space Telescope (JWST) have revealed a hidden population at $z\sim$3-6 with extreme red colours. Taking advantage of the overlap between imaging in the Euclid Deep Fields (EDFs), covering $\sim$ 60 deg$^2$, and ancillary Spitzer observations, we identified 27000 extremely red objects with $H_E-$IRAC2>2.25 (dubbed HIEROs) down to a $10\sigma$ completeness magnitude limit of IRAC2 $=$ 22.5 AB. After a visual inspection to discard artefacts and objects with troubling photometry, we ended up with a final sample of 3900 candidates. We retrieved the physical parameter estimates for these objects from the SED-fitting tool CIGALE. Our results confirm that HIERO galaxies may populate the high-mass end of the stellar mass function at $z>3$, with some reaching extreme stellar masses ($M_*>10^{11}M_\odot$) and exhibiting high dust attenuation ($A_V>3$). However, we consider stellar mass estimates unreliable for $z>3.5$, favouring a lower-z solution. The challenges faced by SED-fitting tools in characterising these objects highlight the need for further studies, incorporating shorter-wavelength and spectroscopic data. Euclid spectra will help resolve degeneracies and better constrain the physical properties of the brightest galaxies. Given the extreme nature of this population, characterising these sources is crucial for understanding galaxy evolution. This work demonstrates Euclid's potential to provide statistical samples of rare, massive, dust-obscured galaxies at $z>3$, which will be prime targets for JWST, ALMA, and ELT.

L. Bisigello, G. Rodighiero, S. Fotopoulou, F. Ricci, K. Jahnke, A. Feltre, V. Allevato, F. Shankar, P. Cassata, E. Dalla Bontà, G. Gandolfi, G. Girardi, M. Giulietti, A. Grazian, C. C. Lovell, R. Maiolino, T. Matamoro Zatarain, M. Mezcua, I. Prandoni, D. Roberts, W. Roster, M. Salvato, M. Siudek, F. Tarsitano, Y. Toba, A. Vietri, L. Wang, G. Zamorani, M. Baes, S. Belladitta, A. Nersesian, L. Spinoglio, X. Lopez Lopez, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, A. Basset, P. Battaglia, R. Bender, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, S. Dusini, A. Ealet, S. Escoffier, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, M. Frailis, E. Franceschi, S. Galeotta, K. George, W. Gillard, B. Gillis, C. Giocoli, P. Gómez-Alvarez, J. Gracia-Carpio, B. R. Granett, F. Grupp, S. Gwyn
0 votes
Paper 76 — arXiv:2503.15323
0 votes
Paper 76 — arXiv:2503.15323

Recent James Webb Space Telescope (JWST) observations have revealed a population of sources with a compact morphology and a `v-shaped' continuum, namely blue at rest-frame $\lambda<4000$A and red at longer wavelengths. The nature of these sources, called `little red dots' (LRDs), is still debated, since it is unclear if they host active galactic nuclei (AGN) and their number seems to drastically drop at z<4. We utilise the 63 $deg^2$ covered by the quick Euclid Quick Data Release (Q1) to extend the search for LRDs to brighter magnitudes and to lower z than what has been possible with JWST to have a broader view of the evolution of this peculiar galaxy population. The selection is done by fitting the available photometric data (Euclid, Spitzer/IRAC, and ground-based griz data) with two power laws, to retrieve the rest-frame optical and UV slopes consistently over a large redshift range (i.e, z<7.6). We exclude extended objects and possible line emitters, and perform a visual inspection to remove imaging artefacts. The final selection includes 3341 LRD candidates from z=0.33 to z=3.6, with 29 detected in IRAC. Their rest-frame UV luminosity function, in contrast with previous JWST studies, shows that the number density of LRD candidates increases from high-z down to z=1.5-2.5 and decreases at even lower z. Less evolution is apparent focusing on the subsample of more robust LRD candidates having IRAC detections, which is affected by low statistics and limited by the IRAC resolution. The comparison with previous quasar UV luminosity functions shows that LRDs are not the dominant AGN population at z<4. Follow-up studies of these LRD candidates are key to confirm their nature, probe their physical properties and check for their compatibility with JWST sources, since the different spatial resolution and wavelength coverage of Euclid and JWST could select different samples of compact sources.

V. Busillo, C. Tortora, R. B. Metcalf, J. W. Nightingale, M. Meneghetti, F. Gentile, R. Gavazzi, F. Zhong, R. Li, B. Clément, G. Covone, N. R. Napolitano, F. Courbin, M. Walmsley, E. Jullo, J. Pearson, D. Scott, A. M. C. Le Brun, L. Leuzzi, N. Aghanim, B. Altieri, A. Amara, S. Andreon, H. Aussel, C. Baccigalupi, M. Baldi, S. Bardelli, P. Battaglia, A. Biviano, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, V. F. Cardone, J. Carretero, S. Casas, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, S. de la Torre, G. De Lucia, A. M. Di Giorgio, J. Dinis, H. Dole, F. Dubath, X. Dupac, S. Dusini, S. Escoffier, M. Farina, R. Farinelli, F. Faustini, S. Ferriol, F. Finelli, S. Fotopoulou, M. Frailis, E. Franceschi, S. Galeotta, K. George, W. Gillard, B. Gillis, C. Giocoli, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, S. V. H. Haugan, W. Holmes, I. Hook, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, B. Joachimi, E. Keihänen, S. Kermiche, A. Kiessling, B. Kubik, M. Kümmel, M. Kunz, H. Kurki-Suonio, Q. Le Boulc'h, S. Ligori, P. B. Lilje, V. Lindholm
0 votes
Paper 82 — arXiv:2503.15329
0 votes
Paper 82 — arXiv:2503.15329

The Euclid mission aims to survey around 14000 deg^{2} of extragalactic sky, providing around 10^{5} gravitational lens images. Modelling of gravitational lenses is fundamental to estimate the total mass of the lens galaxy, along with its dark matter content. Traditional modelling of gravitational lenses is computationally intensive and requires manual input. In this paper, we use a Bayesian neural network, LEns MOdelling with Neural networks (LEMON), for modelling Euclid gravitational lenses with a singular isothermal ellipsoid mass profile. Our method estimates key lens mass profile parameters, such as the Einstein radius, while also predicting the light parameters of foreground galaxies and their uncertainties. We validate LEMON's performance on both mock Euclid data sets, real Euclidised lenses observed with Hubble Space Telescope (hereafter HST), and real Euclid lenses found in the Perseus ERO field, demonstrating the ability of LEMON to predict parameters of both simulated and real lenses. Results show promising accuracy and reliability in predicting the Einstein radius, axis ratio, position angle, effective radius, Sérsic index, and lens magnitude for simulated lens galaxies. The application to real data, including the latest Quick Release 1 strong lens candidates, provides encouraging results, particularly for the Einstein radius. We also verified that LEMON has the potential to accelerate traditional modelling methods, by giving to the classical optimiser the LEMON predictions as starting points, resulting in a speed-up of up to 26 times the original time needed to model a sample of gravitational lenses, a result that would be impossible with randomly initialised guesses. This work represents a significant step towards efficient, automated gravitational lens modelling, which is crucial for handling the large data volumes expected from Euclid.

C. Gouin, C. Laigle, F. Sarron, T. Bonnaire, J. G. Sorce, N. Aghanim, M. Magliocchetti, L. Quilley, P. Boldrini, F. Durret, C. Pichon, U. Kuchner, N. Malavasi, K. Kraljic, R. Gavazzi, Y. Kang, S. A. Stanford, P. Awad, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, A. Basset, P. Battaglia, F. Bernardeau, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, S. de la Torre, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, A. Ealet, S. Escoffier, M. Fabricius, M. Farina, F. Faustini, S. Ferriol, F. Finelli, S. Fotopoulou, M. Frailis, E. Franceschi, S. Galeotta, K. George, B. Gillis, C. Giocoli, P. Gómez-Alvarez, J. Gracia-Carpio, B. R. Granett, A. Grazian, F. Grupp, S. Gwyn, S. V. H. Haugan, W. Holmes, I. M. Hook, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, B. Joachimi, E. Keihänen, S. Kermiche, A. Kiessling, M. Kilbinger, B. Kubik, M. Kümmel, M. Kunz
0 votes
Paper 85 — arXiv:2503.15332
0 votes
Paper 85 — arXiv:2503.15332

The matter distribution around galaxy clusters is distributed over several filaments, reflecting their positions as nodes in the large-scale cosmic web. The number of filaments connected to a cluster, namely its connectivity, is expected to affect the physical properties of clusters. Using the first Euclid galaxy catalogue from the Euclid Quick Release 1 (Q1), we investigate the connectivity of galaxy clusters and how it correlates with their physical and galaxy member properties. Around 220 clusters located within the three fields of Q1 (covering $\sim 63 \ \text{deg}^2$), are analysed in the redshift range $0.2 < z < 0.7$. Due to the photometric redshift uncertainty, we reconstruct the cosmic web skeleton, and measure cluster connectivity, in 2-D projected slices with a thickness of 170 comoving $h^{-1}.\text{Mpc}$ and centred on each cluster redshift, by using two different filament finder algorithms on the most massive galaxies ($M_*\ > 10^{10.3} \ M_\odot$). In agreement with previous measurements, we recover the mass-connectivity relation independently of the filament detection algorithm, showing that the most massive clusters are, on average, connected to a larger number of cosmic filaments, consistent with hierarchical structure formation models. Furthermore, we explore possible correlations between connectivities and two cluster properties: the fraction of early-type galaxies and the Sérsic index of galaxy members. Our result suggests that the clusters populated by early-type galaxies exhibit higher connectivity compared to clusters dominated by late-type galaxies. These preliminary investigations highlight our ability to quantify the impact of the cosmic web connectivity on cluster properties with Euclid.

C. Duffy, E. Cappellaro, M. T. Botticella, I. M. Hook, F. Poidevin, T. J. Moriya, A. A. Chrimes, V. Petrecca, K. Paterson, A. Goobar, L. Galbany, R. Kotak, C. Gall, C. M. Gutierrez, C. Tao, L. Izzo, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, A. Basset, P. Battaglia, A. Biviano, A. Bonchi, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, V. Capobianco, C. Carbone, J. Carretero, R. Casas, S. Casas, M. Castellano, G. Castignani, S. Cavuoti, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice, L. Conversi, Y. Copin, F. Courbin, H. M. Courtois, M. Cropper, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, C. A. J. Duncan, X. Dupac, S. Dusini, A. Ealet, S. Escoffier, M. Farina, F. Faustini, S. Ferriol, S. Fotopoulou, M. Frailis, P. Franzetti, S. Galeotta, K. George, B. Gillis, C. Giocoli, P. Gómez-Alvarez, A. Grazian, F. Grupp, S. Gwyn, S. V. H. Haugan, J. Hoar, H. Hoekstra, W. Holmes, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, E. Keihänen, S. Kermiche, B. Kubik, K. Kuijken, M. Kümmel, M. Kunz, H. Kurki-Suonio, Q. Le Boulc'h, A. M. C. Le Brun, D. Le Mignant, P. Liebing, S. Ligori, P. B. Lilje, V. Lindholm, I. Lloro
0 votes
Paper 87 — arXiv:2503.15334
0 votes
Paper 87 — arXiv:2503.15334

We report on serendipitous \Euclid observations of previously known transients, using the \Euclid Q1 data release. By cross-matching with the Transient Name Server (TNS) we identify 164 transients that coincide with the data release. Although the \Euclid Q1 release only includes single-epoch data, we are able to make \Euclid photometric measurements at the location of 161 of these transients. \Euclid obtained deep photometric measurements or upper limits of these transients in the \IE, \YE, \JE, and \HE bands at various phases of the transient light-curves, including before, during, and after the observations of ground-based transient surveys. Approximately 70\% of known transients reported in the six months before the \Euclid observation date and with discovery magnitude brighter than 24 were detected in \Euclid $\IE$ images. Our observations include one of the earliest near-infrared detections of a Type~Ia supernova (SN~2024pvw) 15~days prior to its peak brightness, and the late-phase (435.9~days post peak) observations of the enigmatic core-collapse SN~2023aew. \Euclid deep photometry provides valuable information on the nature of these transients such as their progenitor systems and power sources, with late time observations being a uniquely powerful contribution. In addition, \Euclid is able to detect the host galaxies of some transients that were previously classed as hostless. The Q1 data demonstrate the power of the \Euclid data even with only single-epoch observations available, as will be the case for much larger areas of sky in the Euclid Wide Survey.

F. R. Marleau, R. Habas, D. Carollo, C. Tortora, P.-A. Duc, E. Sola, T. Saifollahi, M. Fügenschuh, M. Walmsley, R. Zöller, A. Ferré-Mateu, M. Cantiello, M. Urbano, E. Saremi, R. Ragusa, R. Laureijs, M. Hilker, O. Müller, M. Poulain, R. F. Peletier, S. J. Sprenger, O. Marchal, N. Aghanim, B. Altieri, A. Amara, S. Andreon, N. Auricchio, H. Aussel, C. Baccigalupi, M. Baldi, A. Balestra, S. Bardelli, A. Basset, P. Battaglia, R. Bender, A. Biviano, A. Bonchi, D. Bonino, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, G. Cañas-Herrera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, M. Castellano, G. Castignani, S. Cavuoti, K. C. Chambers, A. Cimatti, C. Colodro-Conde, G. Congedo, C. J. Conselice L. Conversi, Y. Copin, L. Corcione, F. Courbin, H. M. Courtois, M. Cropper, J.-C. Cuillandre, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, H. Dole, F. Dubath, X. Dupac, S. Dusini, S. Escoffier, M. Fabricius, M. Farina, F. Faustini, S. Ferriol, P. Fosalba, S. Fotopoulou, M. Frailis, E. Franceschi, P. Franzetti, M. Fumana, S. Galeotta, K. George, B. Gillis, C. Giocoli, B. R. Granett, A. Grazian, F. Grupp, S. Gwyn, S. V. H. Haugan, J. Hoar, H. Hoekstra, W. Holmes, F. Hormuth, A. Hornstrup, P. Hudelot, K. Jahnke, M. Jhabvala, B. Joachimi, E. Keihänen
0 votes
Paper 88 — arXiv:2503.15335
0 votes
Paper 88 — arXiv:2503.15335

The Euclid Q1 fields were selected for calibration purposes in cosmology and are therefore relatively devoid of nearby galaxies. However, this is precisely what makes them interesting fields in which to search for dwarf galaxies in local density environments. We take advantage of the unprecedented depth, spatial resolution, and field of view of the Euclid Quick Release (Q1) to build a census of dwarf galaxies in these regions. We have identified dwarfs in a representative sample of 25 contiguous tiles in the Euclid Deep Field North (EDF-N), covering an area of 14.25 sq. deg. The dwarf candidates were identified using a semi-automatic detection method, based on properties measured by the Euclid pipeline and listed in the MER catalogue. A selection cut in surface brightness and magnitude was used to produce an initial dwarf candidate catalogue, followed by a cut in morphology and colour. This catalogue was visually classified to produce a final sample of dwarf candidates, including their morphology, number of nuclei, globular cluster (GC) richness, and presence of a blue compact centre. We identified 2674 dwarf candidates, corresponding to 188 dwarfs per sq. deg. The visual classification of the dwarfs reveals a slightly uneven morphological mix of 58% ellipticals and 42% irregulars, with very few potentially GC-rich (1.0%) and nucleated (4.0%) candidates but a noticeable fraction (6.9%) of dwarfs with blue compact centres. The distance distribution of 388 (15%) of the dwarfs with spectroscopic redshifts peaks at about 400 Mpc. Their stellar mass distribution confirms that our selection effectively identifies dwarfs while minimising contamination. The most prominent dwarf overdensities are dominated by dEs, while dIs are more evenly distributed. This work highlights Euclid's remarkable ability to detect and characterise dwarf galaxies across diverse masses, distances, and environments.

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We present the progress of work to streamline and simplify the process of exoplanet observation by citizen scientists. International collaborations such as ExoClock and Exoplanet Watch enable citizen scientists to use small telescopes to carry out transit observations. These studies provide essential supports for space missions such as JWST and ARIEL. Contributions include maintenance or recovery of ephemerides, follow up confirmation and transit time variations. Ongoing observation programs benefit from a large pool of observers, with a wide variety of experience levels. Our projects work closely with these communities to streamline their observation pipelines and enable wider participation. Two complementary approaches are taken: Star Guide applies human-centric design and community consultation to identify points of friction within existing systems and provide complementary online tools and resources to reduce barriers to entry to the observing community. Machine Learning is used to accelerate data processing and automate steps which are currently manual, providing a streamlined tool for citizen science and a scalable solution for large-scale archival research.

Aurelio Amerio, Dmitry Malyshev, Bryan Zaldivar, Viviana Gammaldi, Miguel Ángel Sánchez-Conde

We search for dark matter (DM) annihilating subhalos of the Milky Way halo among the Fermi Large Area Telescope (LAT) unassociated sources. We construct, for the first time, a statistical model of the unassociated sources at latitudes above 10 degrees. The latter is built as a combination of both DM annihilation subhalos as well as Galactic and extragalactic astrophysical components. The astrophysical components are constructed based on distributions of associated sources, while the distribution of DM subhalos is derived from Monte Carlo simulations. In this model we take into account the differences in the distributions of associated and unassociated sources including both covariate and prior probability shifts (both being forms of ``dataset shifts''). Previous searches of DM subhalos were based on classify-and-count strategies, while the approach adopted in this work is based on quantification learning, which allows one to determine a well-defined statistical interpretation of the contribution of a population of DM subhalos to the unassociated Fermi-LAT sources. In the $b\bar{b}$ annihilation channel and for a range of DM masses from 10 GeV to 1 TeV, we don't find a significant contribution from DM subhalos and derive a statistical 95% confidence upper limit on the DM annihilation cross section in this channel. While the derived limits are consistent with previous classify-and-count approaches, our generative statistical model opens new avenues for population studies of Fermi-LAT sources and, more generally, for searches of anomalies on top of backgrounds in presence of statistical and systematic uncertainties.

Malte Busmann, Brendan O'Connor, Julian Sommer, Daniel Gruen, Paz Beniamini, Ramandeep Gill, Michael J. Moss, Antonella Palmese, Arno Riffeser, Yu-Han Yang, Eleonora Troja, Simone Dichiara, Roberto Ricci, Noel Klingler, Claus Gössl, Lei Hu, Arne Rau, Christoph Ries, Geoffrey Ryan, Michael Schmidt, Muskan Yadav, Gregory R. Zeimann

Fast X-ray Transients (FXTs) are a rare and poorly understood phenomenon with a variety of possible progenitors. The launch of the Einstein Probe (EP) mission has facilitated a rapid increase in the real-time discovery and follow-up of FXTs. We focus on the recent EP discovered transient EP241021a, which shows a peculiar panchromatic behavior. We obtained optical and near-infrared multi-band imaging and spectroscopy with the Fraunhofer Telescope at Wendelstein Observatory, the Hobby-Eberly Telescope, and the Very Large Telescope over the first 100 days of its evolution. EP241021a was discovered by EP as a soft X-ray trigger, but was not detected at gamma-ray frequencies. The observed soft X-ray prompt emission spectrum is consistent with non-thermal radiation, which requires at least a mildly relativistic outflow with bulk Lorentz factor $\Gamma \gtrsim 4$. The optical and near-infrared lightcurve has a two component behavior where an initially fading component $\sim t^{-1}$ turns to a rise steeper than $\sim t^{4}$ after a few days before peaking at $M_r\approx -22$ mag and quickly returning to the initial decay. The peak absolute magnitude is the most luminous optical emission associated to an FXT, superseding EP240414a. Standard supernova models are unable to reproduce either the absolute magnitude or rapid timescale ($<2$ d) of the rebrightening. The X-ray, optical and near-infrared spectral energy distributions display a red color $r-J\approx 1$ mag, and point to a non-thermal origin ($\nu^{-1}$) for the broadband emission. By considering a gamma-ray burst as a plausible scenario, we favor a refreshed shock as the cause of the rebrightening. This is consistent with the inference of an at least mildly relativistic outflow based on the prompt trigger. Our results suggest a likely link between EP discovered FXTs and low luminosity gamma-ray bursts.

Yumi Choi, Karoline M. Gilbert, Benjamin F. Williams, Daniel R. Weisz, Evan D. Skillman, Julianne J. Dalcanton, Kristen B. W. McQuinn, Andrew E. Dolphin, Giada Pastorelli, Martha L. Boyer, Karl D. Gordon, L'eo Girardi, Maude Gull

We present the star formation histories (SFHs) of ten metal-poor (<12% Zsun), star-forming dwarf galaxies from the Local Ultraviolet to Infrared Treasury (LUVIT) survey. The derived SFHs exhibit significant variability, consistent with the irregular star formation expected for dwarf galaxies. Using synthetic near ultraviolet (UV) and optical CMDs with various yet targeted configurations for dust and input SFHs, we quantitatively demonstrate that simultaneous modeling of the UV and optical CMDs ("UVopt" case) improves the precision of SFH measurements in recent time bins up to ~1 Gyr, compared to the classical single optical CMD modeling ("Opt-only" case). The UVopt case reduces uncertainties relative to the Opt-only case by ~4-8% over the past 10 Myr, ~8-20% over 100 Myr, and ~8-14% over 1 Gyr, across various dust configurations and input SFHs. Additionally, we demonstrate discrepancies in stellar models for blue core helium-burning (BHeB) stars at the low metallicity regime. This discrepancy can artificially inflate star formation rate (SFR) estimates in younger age bins by misinterpreting the evolved BHeB stars as reddened upper main-sequence (MS) stars. Incorporating UV data improves BHeB-MS separation and mitigates the limitations of current low metallicity stellar models. Comparisons of the UVopt SFHs with Ha and FUV-based SFRs reconfirm that Ha is an unreliable tracer over its nominal 10 Myr timescale for low-SFR galaxies, while FUV provides a more reliable tracer but yields SFR_FUV values up to twice those of CMD-based <SFR>_100Myr. Our findings underscore the importance of UV data in refining recent SFHs in low-metallicity environments.

We investigate the optimal approach for recovering the star formation histories (SFHs) and spatial distribution of stellar mass in high-redshift galaxies ($z\sim 2-5$), focusing on the impact of assumed SFH models on derived galaxy properties. Utilizing pixel-by-pixel spectral energy distribution (SED) fitting of multi-band photometry, we explore various parametric SFH models (including exponentially declining ($\tau$), delayed-$\tau$, lognormal, and double-power law) alongside spatially resolved non-parametric methods. We first analyze the models using simulated galaxies and then apply them to observed galaxies for validation and as proof of concept, with additional comparisons to results from unresolved SED fitting. Our findings demonstrate that pixel-by-pixel analysis with parametric models is particularly robust in recovering the true SFHs of simulated galaxies, with the double-power law model outperforming others, including non-parametric methods. This model excels in detecting recent starbursts within the last 500 Myr and capturing the stochastic nature of star formation. Conversely, unresolved photometry with simplistic parametric models tends to produce biased estimates of key galaxy properties, particularly underestimating early star formation. Non-parametric methods, resolved or unresolved, typically yield older mass-weighted ages. Biases in early-time SFRs, likely introduced by prior assumptions, further complicate these models. We conclude that the double-power law model, applied in a pixel-by-pixel framework, offers the most reliable recovery of SFHs and produces robust stellar mass maps. Resolved methods simplify modeling dust and metallicity, enhancing parameter interpretability and underscoring the value of flexible parametric models in spatially resolved analyses.

Mayusree Das (IISc), Armen Sedrakian (Wroclaw/FIAS), Banibrata Mukhopadhyay (IISc)

We present a first two-dimensional general-relativistic analysis of superconducting regions in axially symmetric highly magnetized neutron star (magnetar) models with toroidal magnetic fields. We investigate the topology and distribution of type-II and type-I superconducting regions for varying toroidal magnetic field strengths and stellar masses by solving the Einstein-Maxwell equations using the XNS code. Our results reveal that the outer cores of low- to intermediate-mass magnetars sustain superconductivity over larger regions compared to higher-mass stars with non-trivial distribution of type-II and type-I regions. Consistent with previous one-dimensional (1D) models, we find that regardless of the gravitational mass, the inner cores of magnetars with toroidal magnetic fields are devoid of $S$-wave proton superconductivity. Furthermore, these models contain non-superconducting, torus-shaped regions - a novel feature absent in previous 1D studies. Finally, we speculate on the potential indirect effects of superconductivity on continuous gravitational wave emissions from millisecond pulsars, such as PSR J1843-1113, highlighting their relevance for future gravitational wave detectors.

Vignesh Vaikundaraman, Joanna Drazkowska, Fabian Binkert, Til Birnstiel, Anna Miotello

The inner Solar System is depleted in refractory carbon in comparison to the interstellar medium and the depletion likely took place in the protoplanetary disk phase of the Solar System. We study the effect of photolysis of refractory carbon in the upper layers of the protosolar disk and its interplay with dust collisional growth and vertical mixing. We make use of a 1D Monte Carlo model to simulate dust coagulation and vertical mixing. To model the FUV flux of the disk, we use a simple analytical prescription and benchmark it with data from a radiative transfer simulation. We study the effects of fragmentation and bouncing on dust distribution and the propagation of carbon depletion. We find that when bouncing is included, the size distribution is truncated at smaller sizes than fragmentation-limited size distributions but there is a loss of small grains as well. The population of small grains is reduced due to fewer fragmentation events and this reduces the effectiveness of photolysis. We find that dust collisional growth and vertical mixing increase the effectiveness of carbon depletion by efficiently replenishing carbon to the upper regions of the disk with higher FUV flux. It takes around 100-300 kyr to reach the measured carbon abundances at 1 au, depending on the strength of the turbulence in the disk. These timescales are faster than reported by previous studies. Collisional redistribution and turbulent mixing are important aspects of dust evolution that should be included when modeling dust chemistry as they can influence the efficiency of chemical processes. Photolysis, along with another process such as sublimation, most likely played a key role in refractory carbon depletion that we see around us in the inner Solar System.

Dany Atallah, Yonadav Barry Ginat, Newlin C. Weatherford

Gaia observations have revealed over a million stellar binary candidates within ~1 kpc of the Sun, predominantly characterized by orbital separations >10^3 AU and eccentricities >0.7. The prevalence of such wide, eccentric binaries has proven challenging to explain through canonical binary formation channels. However, recent advances in our understanding of three-body binary formation (3BBF) -- new binary assembly by the gravitational scattering of three unbound bodies -- have shown that 3BBF in star clusters can efficiently generate wide, highly eccentric binaries. We further explore this possibility by constructing a semi-analytic model of the Galactic binary population in the solar neighborhood, originating from 3BBF in star clusters. The model relies on 3BBF scattering experiments to determine how the 3BBF rate and resulting binary properties scale with local stellar density and velocity dispersion. We then model the Galactic stellar-cluster population, incorporating up-to-date prescriptions for the Galaxy's star-formation history as well as the birth properties and internal evolution of its star clusters. Finally, we account for binary destruction induced by perturbations from stellar interactions before cluster escape and and for subsequent changes to binary orbital elements by dynamical interactions in the Galactic field. Without any explicit fine-tuning, our model closely reproduces both the total number of Gaia's wide binaries and their separation distribution, and qualitatively matches the eccentricity distribution, suggesting that 3BBF may be an important formation channel for these enigmatic systems.

Isaiah I. Tristan, Rachel A. Osten, Yuta Notsu, Adam F. Kowalski, Alexander Brown, Graeme L. White, Carol A. Grady, Todd J. Henry, Eliot Halley Vrijmoet

M dwarfs are the most common type of star in the solar neighborhood, and many exhibit frequent and highly energetic flares. To better understand these events across the electromagnetic spectrum, a campaign observed AU Mic (dM1e) over 7 days from the X-ray to radio regimes. Here, we present high-time-resolution light curves from the Karl G. Jansky Very Large Array (VLA) Ku band (12--18 GHz) and the Australia Telescope Compact Array (ATCA) K band (16--25 GHz), which observe gyrosynchrotron radiation and directly probe the action of accelerated electrons within flaring loops. Observations reveal 16 VLA and 3 ATCA flares of varying shapes and sizes, from a short (30 sec) spiky burst to a long-duration ($\sim$5 hr) decaying exponential. The Ku-band spectral index is found to often evolve during flares. Both rising and falling spectra are observed in the Ku-band, indicating optically thick and thin flares, respectively. Estimations from optically thick radiation indicate higher loop-top magnetic field strengths ($\sim$1 kG) and sustained electron densities ($\sim$10$^{6}$ cm$^{-3}$) than previous observations of large M-dwarf flares. We estimate the total kinetic energies of gyrating electrons in optically thin flares to be between 10$^{32}$ and 10$^{34}$ erg when the local magnetic field strength is between 500 and 700 G. These energies are able to explain the combined radiated energies from multi-wavelength observations. Overall, values are more aligned with modern radiative-hydrodynamic simulations of M-dwarf flares, and future modeling efforts will better constrain findings.

F. R. Ferraro, L. Chiappino, A. Bartolomei, L. Origlia, C. Fanelli, B. Lanzoni, C. Pallanca, M. Loriga, S. Leanza, E. Valenti, D. Romano, A. Mucciarelli, D. Massari, M. Cadelano, E. Dalessandro, C. Crociati, R.M.Rich

We present the scientific goals and the very first results of the Bulge Cluster Origin (BulCO) survey. This survey has been specifically designed to perform an unprecedented chemical screening of stellar systems orbiting the Milky Way bulge, with the aim to unveil their true origin. It takes advantage of the improved performances of the spectrograph CRIRES+ operating at the ESO Very Large telescope, in the near-infrared domain. Due to the complex evolutionary history of the Milky Way, a variety of relics tracing different phenomena is expected to populate the Bulge: globular clusters formed in-situ or accreted from outside the Galaxy, nuclear star clusters of cannibalized structures, and possibly a few remnants of the proto-bulge formation process (the so-called ``bulge fossil fragments"). The signatures of the different origins are imprinted in the chemical properties of these stellar systems because specific abundance patterns provide authentic "chemical DNA" tests univocally tracing the enrichment process and, therefore, the environment where the stellar population formed. Thus, each system can provide a new piece of information on the bulge formation and evolutionary history. As first results of the survey, here we discuss the alpha-element and iron abundances of a sample of stars observed in the stellar system Liller 1, which is proposed to be a bulge fossil fragment. By combining this dataset with a recently published sample of high/mid-resolution spectra, we discuss the overall chemical properties of the stellar populations in Liller1, proving its link with the Galactic bulge and providing new constraints on its star formation history.

The secondary/primary cosmic-ray ratios and the diffuse backgrounds of gamma rays and neutrinos provide us with complementary information about the transport of Galactic cosmic rays. We use the recent measurement of the diffuse gamma ray background in the $\sim \rm TeV -\rm PeV$ range by LHAASO and of the very high energy diffuse neutrino background from the Galactic disc by IceCube to show that CRs may be accumulating an approximately energy independent grammage $X\sim 0.4\, \rm g \, \rm cm^{-2}$, in regions where gamma rays and neutrinos are produced with a hard spectrum, resembling the source spectrum. We speculate that this grammage reflects the early stages of cosmic ray transport around sources, in so-called cocoons, where particles spend $\sim 0.3\, \rm Myr$ before starting their journey in the Galactic environment.

In this research note I update the associations between globular clusters and their putative galaxy progenitors determined in Massari et al. (2019), based on the kinematic measurements from the Gaia early data release 3 (eDR3, Gaia Collaboration et al. 2021). The table with the associations is available at this https URL, and will be kept up-to-date whenever improved data become available. The same table will also provide updated age estimates from the CARMA project (see Massari et al. 2023). Please cite this Note alongside Massari, Koppelman & Helmi 2019, eDR3 edition.

A. Jaradat, G. Molera Calvés, J. Edwards, S. Ellingsen, T. McCarthy, J. Morgan

Advancements in VLBI instrumentation, driven by the geodetic community's goal of achieving positioning accuracy of 1 mm and stability of 0.1 mm/y, have led to the development of new broadband systems. Here, we assess the potential of these new capabilities for space weather monitoring. These enhanced VLBI capabilities were used to investigate interplanetary scintillation (IPS), a phenomenon caused by the scattering of radio waves due to density irregularities in the solar wind. Compact radio sources near the Sun were observed using the AuScope VLBI array in Australia, which consists of 12-meter telescopes at Hobart, Katherine, and Yarragadee. The baseline lengths between these telescopes are approximately 3400 km (Hobart-Katherine), 3200 km (Hobart-Yarragadee), and 2400 km (Katherine-Yarragadee). The observations covered solar elongations from 6.5$^\circ$ to 11.3$^\circ$ and frequencies between 3 and 13 GHz. The study focused on phase scintillation as an indicator of turbulence in the solar wind. As the solar elongation decreased, we observed an increase in the phase scintillation index, consistent with theoretical models. Importantly, the broadband system also detected IPS using relatively weak radio sources. Additionally, the phase scintillation increased with baseline length, in agreement with Kolmogorov turbulence with an index of 11/3. These findings demonstrate the effectiveness of geodetic broadband VLBI in capturing detailed features of the solar wind. This capability enables continuous space weather monitoring and advances our understanding of solar and interplanetary dynamics.

Gravitational waves (GWs) from compact binary coalescences (CBCs) provide a new avenue to probe the cosmic expansion, in particular the Hubble constant $H_0$. The spectral sirens method is one of the most used techniques for GW cosmology. It consists of obtaining cosmological information from the GW luminosity distance, directly inferred from data, and the redshift that can be implicitly obtained from the source frame mass distribution of the CBC population. With GW detectors, populations of CBCs can be either observed as resolved individual sources or implicitly as a stochastic gravitational-wave background (SGWB) from the unresolved ones. In this manuscript, we study how resolved and unresolved sources of CBCs can be employed in the spectral siren framework to constrain cosmic expansion. The idea stems from the fact that the SGWB can constrain additional population properties of the CBCs thus potentially improving the measurement precision of the cosmic expansion parameters. We show that with a 5-detector network at O5-designed sensitivity, the inclusion of the SGWB will improve our ability to exclude low values of $H_0$ and the dark matter energy fraction $\Omega_m$, while also improving the determination of a possible CBC peak in redshift. Although low values of $H_0$ and $\Omega_m$ will be better constrained, we obtain that most on the precsion on $H_0$ will be provided by resolved spectral sirens. We also performed a spectral siren analysis for 59 resolved binary black hole sources detected during the third observing run with an inverse false alarm rate higher than 1 per year jointly with the SGWB. We obtain that with current sensitivities, the cosmological and population results are not impacted by the inclusion of the SGWB.

Sarah A. Brands, Frank Backs, Alex de Koter, Joachim Puls, Paul A. Crowther, Hugues Sana, Frank Tramper, Lex Kaper, Jon O. Sundqvist, Joachim M. Bestenlehner, Florian A. Driessen, Christiana Erba, Calum Hawcroft, Artemio Herrero, D. John Hillier, Richard Ignace, Roel R. Lefever, N. Dylan Kee, Laurent Mahy, Antony F.J. Moffat, Francisco Najarro, Raman Prinja, Varsha Ramachandran, Andreas A.C. Sander, Jorick S. Vink, the XShootU collaboration

Mass loss governs the evolution of massive stars and shapes the stellar surroundings. To quantify the impact of the stellar winds we need to know the exact mass-loss rates; however, empirical constraints on the rates are hampered by limited knowledge of their small-scale wind structure or 'wind clumping'. We aim to improve empirical constraints on the mass loss of massive stars by investigating the clumping properties of their winds, in particular the relation between stellar parameters and wind structure. We analyse the optical and ultraviolet spectra of 25 O-type (super)giants in the LMC, using the model atmosphere code Fastwind and a genetic algorithm. We derive stellar and wind parameters including detailed clumping properties, such as the amount of clumping, the density of the interclump medium, velocity-porosity of the medium, and wind turbulence. We obtain stellar and wind parameters for 24 of our sample stars and find that the winds are highly clumped, with an average clumping factor of $f_{\rm cl}=33\pm14$, an interclump density factor of $f_{\rm ic}=0.2\pm0.1$, and moderate to strong velocity-porosity effects. The scatter around the average values of the wind-structure parameters is large. With the exception of a significant, positive correlation between the interclump density factor and mass loss, we find no dependence of clumping parameters on either mass-loss rate or stellar properties. In the luminosity range that we investigate, the empirical and theoretical mass-loss rates both have a scatter of about 0.5~dex, or a factor 3. Within this uncertainty, the empirical rates and the theoretical predictions agree. The origin of the scatter of the empirical mass-loss rates requires further investigation. It is possible that our description of wind clumping is still not sufficient to capture effects of the structured wind; this could contribute to the scatter.

Kyle Van Gorkom, Ramya M. Anche, Christopher B. Mendillo, Jessica Gersh-Range, Justin Hom, Tyler D Robinson, Mamadou N'Diaye, Nikole K. Lewis, Bruce Macintosh, Ewan S. Douglas

NASA's Habitable Worlds Observatory (HWO) concept and the 2020 Decadal Survey's recommendation to develop a large space telescope to "detect and characterize Earth-like extrasolar planets" requires new starlight suppression technologies to probe a variety of biomarkers across multiple wavelengths. Broadband absorption due to ozone dominates Earth's spectrum in the mid-ultraviolet (200-300 nm) and can be detected with low spectral resolution. Despite the high value of direct ultraviolet (UV) exoplanet observations, high-contrast coronagraph demonstrations have yet to be performed in the UV. Typical coronagraph leakage sources such as wavefront error, surface scatter, polarization aberrations, and coronagraph mask quality all become more significant in the UV and threaten the viability of HWO to produce meaningful science in this regime. As a first step toward a demonstration of UV coronagraphy in a laboratory environment, we develop an end-to-end model to produce performance predictions and a contrast budget for a vacuum testbed operating at wavelengths from 200-400nm. At 300nm, our model predicts testbed performance of ${\sim}3\times10^{-9}$ contrast in a narrow 2% bandwidth and $\lessapprox10^{-8}$ in a 5% bandwidth, dominated primarily by the chromatic residuals from surface errors on optics that are not conjugate to the pupil.

Junehyoung Jeon, Boyuan Liu, Anthony J. Taylor, Vasily Kokorev, John Chisholm, Dale D. Kocevski, Steven L. Finkelstein, Volker Bromm

Observations with the James Webb Space Telescope (JWST) have identified an abundant population of supermassive black holes (SMBHs) already in place during the first few hundred million years of cosmic history. Most of them appear overmassive relative to the stellar mass in their host systems, challenging models of early black hole seeding and growth. Multiple pathways exist to explain their formation, including heavy seeds formed from direct collapse/supermassive stars or sustained super-Eddington accretion onto light stellar remnant seeds. We use the semi-analytical code A-SLOTH to predict the emerging SMBH mass function under physically motivated models for both light and heavy seed formation, to be compared with upcoming ultra-deep JWST surveys. We find that both pathways can reproduce observations at $z\sim5-6$, but have distinct features at higher redshifts of $z\sim10$. Specifically, JWST observations have the potential to constrain the fraction of efficiently accreting (super-Eddington) SMBHs, as well as the existence and prevalence of heavy seeds, in particular through ultra-deep observations of blank fields and/or gravitational lensing surveys. Such observations will provide key insights to understand the process of SMBH formation and evolution during the emergence of the first galaxies. We further emphasize the great promise of possible SMBH detections at $z\gtrsim 15$ with future JWST observations to break the degeneracy between light- and heavy-seed models.

Bo Huang, Josep M. Girart, Ian W. Stephens, Philip C. Myers, Qizhou Zhang, Paulo Cortés, Álvaro Sánchez-Monge, Manuel Fernández-López, Valentine J. M. Le Gouellec, Tom Megeath, Nadia M. Murillo, John M. Carpenter, Zhi-Yun Li, Junhao Liu, Leslie W. Looney, Sarah Sadavoy, Nicole Karnath, Woojin Kwon

The {\em B}-field Orion Protostellar Survey (BOPS) recently obtained polarimetric observations at 870 ${\rm \mu m}$ towards 61 protostars in the Orion molecular clouds with $\sim 1^{\prime\prime}$ spatial resolution using the Atacama Large Millimeter/submillimeter Array. From the BOPS sample, we selected the 26 protostars with extended polarized emission within a radius of $\sim 6^{\prime\prime}$ (2400~au) around the protostar. This allows to have sufficient statistical polarization data to infer the magnetic field strength. The magnetic field strength is derived using the Davis-Chandrasekhar-Fermi method. The underlying magnetic field strengths are approximately 2.0~mG for protostars with a standard hourglass magnetic field morphology, which is higher than the values derived for protostars with rotated hourglass, spiral, and complex magnetic field configurations ($\lesssim1.0$~mG). This suggests that the magnetic field plays a more significant role in envelopes exhibiting a standard hourglass field morphology, and a value of $\gtrsim2.0$ mG would be required to maintain such a structure at these scales. Furthermore, most protostars in the sample are slightly supercritical, with mass-to-flux ratios $\lesssim3.0$. In particular, the mass-to-flux ratios for all protostars with a standard hourglass magnetic field morphology are lower than 3.0. However, these ratios do not account for the contribution of the protostellar mass, which means they are likely significantly underestimated.

Catherine Gallagher, Tariq Yasin, Richard Stiskalek, Harry Desmond, Matt J. Jarvis

The evolution of galaxies is known to be connected to their position within the large-scale structure and their local environmental density. We investigate the relative importance of these using the underlying dark matter density field extracted from the Constrained Simulations in BORG (CSiBORG) suite of constrained cosmological simulations. We define cosmic web environment through both dark matter densities averaged on a scale up to 16 Mpc/h, and through cosmic web location identified by applying DisPerSE to the CSiBORG haloes. We correlate these environmental measures with the properties of observed galaxies in large surveys using optical data (from the NASA-Sloan Atlas) and 21-cm radio data (from ALFALFA). We find statistically significant correlations between environment and colour, neutral hydrogen gas (HI) mass fraction, star formation rate and Sérsic index. Together, these correlations suggest that bluer, star forming, HI rich, and disk-type galaxies tend to reside in lower density areas, further from filaments, while redder, more elliptical galaxies with lower star formation rates tend to be found in higher density areas, closer to filaments. We find analogous trends with the quenching of galaxies, but notably find that the quenching of low mass galaxies has a greater dependence on environment than the quenching of high mass galaxies. We find that the relationship between galaxy properties and the environmental density is stronger than that with distance to filament, suggesting that environmental density has a greater impact on the properties of galaxies than their location within the larger-scale cosmic web.

L. Casas, H. K. Herrera-Alcantar, J. Chaves-Montero, A. Cuceu, A. Font-Ribera, M. Lokken, M. Abdul Karim, C. Ramírez-Pérez, J. Aguilar, S. Ahlen, U. Andrade, E. Armengaud, A. Aviles, S. Bailey, S. BenZvi, D. Bianchi, A. Brodzeller, D. Brooks, R. Canning, A. Carnero Rosell, M. Charles, E. Chaussidon, T. Claybaugh, K. S. Dawson, A. de la Macorra, A. de Mattia, Arjun Dey, Biprateep Dey, Z. Ding, P. Doel, D. J. Eisenstein, W. Elbers, S. Ferraro, J. E. Forero-Romero, C. Garcia-Quintero, Lehman H. Garrison, E. Gaztañaga, H. Gil-Marín, S. Gontcho A Gontcho, A. X. Gonzalez-Morales, C. Gordon, G. Gutierrez, J. Guy, M. Herbold, K. Honscheid, C. Howlett, D. Huterer, M. Ishak, S. Juneau, R. Kehoe, D. Kirkby, T. Kisner, A. Kremin, O. Lahav, M. Landriau, J.M. Le Goff, L. Le Guillou, A. Leauthaud, M. E. Levi, Q. Li, M. Manera, P. Martini, A. Meisner, J. Mena-Fernández, R. Miquel, J. Moustakas, D. Muñoz Santos, A. D. Myers, S. Nadathur, L. Napolitano, G. Niz, H. E. Noriega, E. Paillas, N. Palanque-Delabrouille, W. J. Percival, Matthew M. Pieri, C. Poppett, F. Prada, I. Pérez-Ràfols, C. Ravoux, G. Rossi, E. Sanchez, D. Schlegel, M. Schubnell, H. Seo, F. Sinigaglia, D. Sprayberry, T. Tan, G. Tarlé, P. Taylor, W. Turner, M. Vargas-Magaña, M. Walther, B. A. Weaver, M. Wolfson, C. Yèche, P. Zarrouk, R. Zhou

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The second data release (DR2) of the Dark Energy Spectroscopic Instrument (DESI), containing data from the first three years of observations, doubles the number of Lyman-$\alpha$ (Ly$\alpha$) forest spectra in DR1 and it provides the largest dataset of its kind. To ensure a robust validation of the Baryonic Acoustic Oscillation (BAO) analysis using Ly$\alpha$ forests, we have made significant updates compared to DR1 to both the mocks and the analysis framework used in the validation. In particular, we present CoLoRe-QL, a new set of Ly$\alpha$ mocks that use a quasi-linear input power spectrum to incorporate the non-linear broadening of the BAO peak. We have also increased the number of realisations used in the validation to 400, compared to the 150 realisations used in DR1. Finally, we present a detailed study of the impact of quasar redshift errors on the BAO measurement, and we compare different strategies to mask Damped Lyman-$\alpha$ Absorbers (DLAs) in our spectra. The BAO measurement from the Ly$\alpha$ dataset of DESI DR2 is presented in a companion publication.

W. Elbers, A. Aviles, H. E. Noriega, D. Chebat, A. Menegas, C. S. Frenk, C. Garcia-Quintero, D. Gonzalez, M. Ishak, O. Lahav, K. Naidoo, G. Niz, C. Yèche, M. Abdul Karim, S. Ahlen, O. Alves, U. Andrade, E. Armengaud, D. Bianchi, S. Brieden, A. Brodzeller, D. Brooks, E. Burtin, R. Calderon, R. Canning, A. Carnero Rosell, L. Casas, F. J. Castander, M. Charles, E. Chaussidon, J. Chaves-Montero, T. Claybaugh, S. Cole, A. Cuceu, K. S. Dawson, A. de la Macorra, A. de Mattia, N. Deiosso, A. Dey, B. Dey, Z. Ding, P. Doel, D. J. Eisenstein, S. Ferraro, A. Font-Ribera, J. E. Forero-Romero, L. H. Garrison, E. Gaztañaga, H. Gil-Marín, A. X. Gonzalez-Morales, G. Gutierrez, S. He, M. Herbold, H. K. Herrera-Alcantar, C. Howlett, D. Huterer, R. Kehoe, D. Kirkby, T. Kisner, A. Kremin, C. Lamman, M. Landriau, L. Le Guillou, A. Leauthaud, M. E. Levi, Q. Li, K. Lodha, C. Magneville, M. Manera, W. L. Matthewson, A. Meisner, R. Miquel, J. Moustakas, S. Nadathur, J. A. Newman, E. Paillas, N. Palanque-Delabrouille, W. J. Percival, M. M. Pieri, F. Prada, I. Pérez-Ràfols, D. Rabinowitz, C. Ramírez-Pérez, M. Rashkovetskyi, C. Ravoux, H. Rivera, J. Rohlf, G. Rossi, V. Ruhlmann-Kleider, L. Samushia, E. Sanchez, D. Schlegel, M. Schubnell, F. Sinigaglia, D. Sprayberry, T. Tan, G. Tarlé, P. Taylor, W. Turner, M. Vargas-Magaña

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The Dark Energy Spectroscopic Instrument (DESI) Collaboration has obtained robust measurements of baryon acoustic oscillations (BAO) in the redshift range, $0.1 < z < 4.2$, based on the Lyman-$\alpha$ forest and galaxies from Data Release 2 (DR2). We combine these measurements with external cosmic microwave background (CMB) data from Planck and ACT to place our tightest constraints yet on the sum of neutrino masses. Assuming the cosmological $\Lambda$CDM model and three degenerate neutrino states, we find $\sum m_\nu<0.0642$ eV (95%). When accounting for neutrino oscillation constraints, we find a preference for the normal mass ordering and an upper bound of $m_l < 0.023$ eV (95%) on the lightest neutrino mass. However, we determine using frequentist and Bayesian methods that our constraints are in moderate tension with the lower limits derived from neutrino oscillations. Correcting for the physical boundary at zero mass, we report a 95% Feldman-Cousins upper bound of $\sum m_\nu<0.053$ eV, breaching the lower limit from neutrino oscillations. Considering a more general Bayesian analysis with an effective cosmological neutrino mass parameter, $\sum m_{\nu,\mathrm{eff}}$, that allows for negative energy densities and removes unsatisfactory prior weight effects, we derive constraints that are in $3\sigma$ tension with the same oscillation limit. In the absence of unknown systematics, this finding could be interpreted as a hint of new physics not necessarily related to neutrinos. The preference of DESI and CMB data for an evolving dark energy model offers one possible solution. In the $w_0w_a$CDM model, we find $\sum m_\nu<0.163$ eV (95%), resolving the neutrino tension. [Abridged]

M. Abdul Karim, A. G. Adame, D. Aguado, J. Aguilar, S. Ahlen, S. Alam, G. Aldering, D. M. Alexander, R. Alfarsy, L. Allen, C. Allende Prieto, O. Alves, A. Anand, U. Andrade, E. Armengaud, S. Avila, A. Aviles, H. Awan, S. Bailey, A. Baleato Lizancos, O. Ballester, A. Bault, J. Bautista, S. BenZvi, L. Beraldo e Silva, J. R. Bermejo-Climent, F. Beutler, D. Bianchi, C. Blake, R. Blum, A. S. Bolton, M. Bonici, S. Brieden, A. Brodzeller, D. Brooks, E. Buckley-Geer, E. Burtin, R. Canning, A. Carnero Rosell, A. Carr, P. Carrilho, L. Casas, F. J. Castander, R. Cereskaite, J. L. Cervantes-Cota, E. Chaussidon, J. Chaves-Montero, S. Chen, X. Chen, T. Claybaugh, S. Cole, A. P. Cooper, M.-C. Cousinou, A. Cuceu, T. M. Davis, K. S. Dawson, R. de Belsunce, R. de la Cruz, A. de la Macorra, A. de Mattia, N. Deiosso, J. Della Costa, R. Demina, U. Demirbozan, J. DeRose, A. Dey, B. Dey, J. Ding, Z. Ding, P. Doel, K. Douglass, M. Dowicz, H. Ebina, J. Edelstein, D. J. Eisenstein, W. Elbers, N. Emas, S. Escoffier, P. Fagrelius, X. Fan, K. Fanning, V. A. Fawcett, E. Fernández-García, S. Ferraro, N. Findlay, A. Font-Ribera, J. E. Forero-Romero, D. Forero-Sánchez, C. S. Frenk, B. T. Gänsicke, L. Galbany, J. García-Bellido, C. Garcia-Quintero, L. H. Garrison, E. Gaztañaga, H. Gil-Marín, O. Y. Gnedin, S. Gontcho A Gontcho, A. X. Gonzalez-Morales

In 2021 May the Dark Energy Spectroscopic Instrument (DESI) collaboration began a 5-year spectroscopic redshift survey to produce a detailed map of the evolving three-dimensional structure of the universe between $z=0$ and $z\approx4$. DESI's principle scientific objectives are to place precise constraints on the equation of state of dark energy, the gravitationally driven growth of large-scale structure, and the sum of the neutrino masses, and to explore the observational signatures of primordial inflation. We present DESI Data Release 1 (DR1), which consists of all data acquired during the first 13 months of the DESI main survey, as well as a uniform reprocessing of the DESI Survey Validation data which was previously made public in the DESI Early Data Release. The DR1 main survey includes high-confidence redshifts for 18.7M objects, of which 13.1M are spectroscopically classified as galaxies, 1.6M as quasars, and 4M as stars, making DR1 the largest sample of extragalactic redshifts ever assembled. We summarize the DR1 observations, the spectroscopic data-reduction pipeline and data products, large-scale structure catalogs, value-added catalogs, and describe how to access and interact with the data. In addition to fulfilling its core cosmological objectives with unprecedented precision, we expect DR1 to enable a wide range of transformational astrophysical studies and discoveries.

Cheongho Han, Weicheng Zang, Andrzej Udalski, Chung-Uk Lee, Ian A. Bond, Yongxin Wen, Bo Ma, Michael D. Albrow, Sun-Ju Chung, Andrew Gould, Kyu-Ha Hwang, Youn Kil Jung, Yoon-Hyun Ryu, Yossi Shvartzvald, In-Gu Shin, Hongjing Yang, Jennifer C. Yee, Doeon Kim, Dong-Jin Kim, Sang-Mok Cha, Seung-Lee Kim, Dong-Joo Lee, Yongseok Lee, Byeong-Gon Park, Richard W. Pogge, Przemek Mróz, Michał K. Szymański, Jan Skowron, Radosław Poleski, Igor Soszyński, Paweł Pietrukowicz, Szymon Kozłowski, Krzysztof A. Rybicki, Patryk Iwanek, Krzysztof Ulaczyk, Marcin Wrona, Mariusz Gromadzki, Mateusz J. Mróz, Fumio Abe, Ken Bando, David P. Bennett, Aparna Bhattacharya, Akihiko Fukui, Ryusei Hamada, Shunya Hamada, Naoto Hamasaki, Yuki Hirao, Stela Ishitani Silva, Naoki Koshimoto, Yutaka Matsubara, Shota Miyazaki, Yasushi Muraki, Tutumi Nagai, Kansuke Nunota, Greg Olmschenk, Clément Ranc, Nicholas J. Rattenbury, Yuki Satoh, Takahiro Sumi, Daisuke Suzuki, Sean K. Terry, Paul J. Tristram, Aikaterini Vandorou, Hibiki Yama

The United Kingdom Infrared Telescope (UKIRT) microlensing survey was conducted over four years, from 2016 to 2019, with the goal of serving as a precursor to future near-infrared microlensing surveys (Shvartzvald et al. 2017). Focusing on stars in the Galactic center and utilizing near-infrared passbands, the survey identified approximately one thousand microlensing events, 27 of which displayed anomalies in their light curves (Wen et al. 2023). This paper presents an analysis of these anomalous events, aiming to uncover the underlying causes of the observed anomalies. The events were analyzed under various configurations, considering the potential binarity of both the lens and the source. For 11 events that were additionally observed by other optical microlensing surveys, including those conducted by the OGLE, KMTNet, and MOA collaborations, we incorporated their data into our analysis. Among the reported anomalous events, we revealed the nature of 24 events except for three events, in which one was likely to be a transient variable, and two were were difficult to accurately characterize their nature due to the limitations of the available data. We confirmed the binary lens nature of the anomalies in 22 events. Among these, we verified the earlier discovery that the companion in the binary lens system UKIRT11L is a planetary object. Accurately describing the anomaly in UKIRT21 required a model that accounted for the binarity of both the lens and the source. For two events UKIRT01 and UKIRT17, the anomalies could be interpreted using either a binary-source or a binary-lens model.

The chemical composition of the Sun is still a highly controversial issue. No solar model has yet been able to simultaneously reproduce the solar lithium and beryllium abundances, along with helioseismic results, including the rotation profile. Lithium and beryllium are fragile elements that are highly sensitive to the physical conditions, as well as to transport and mixing processes within and below the convective zone (CZ). Uncovering the transport mechanisms responsible for the depletion of Li and Be in the Sun is crucial for using them as tools to understand stellar interiors and the associated transport and mixing processes. We constructed rotating solar models based on Magg's abundance scale, incorporating the effects of convective overshoot and magnetic fields. The rotating model exhibits superior sound speed and density profile and successfully reproduces the observed ratios $r_{02}$ and $r_{13}$. It also matches the seismically inferred CZ depth, surface helium abundance, and rotation profile, as well as the detected Li and Be abundances and neutrino fluxes within $1\sigma$. The depletion of Li is dominated by convective overshoot and rotational mixing, while Be depletion is primarily driven by gravitational settling and rotational mixing. The presence of the tachocline accelerates Li depletion but slows down Be depletion. These distinct depletion mechanisms result in the surface abundances of Li and Be evolving differently over time.

The stellar initial mass function is of great significance for the study of star formation and galactic structure. Observations indicate that the IMF follows a power-law form. This work derived that when the expected number of stars formed from a spherical molecular cloud is much greater than 1, there is a relationship between the slope $\alpha$ of the IMF and $r^n$ in the radius-density relation of spherically symmetric gas clouds, given by $\alpha = 3/(n+3)$ ($\Gamma_{\mathrm {IMF}} = n/(n+3)$). This conclusion is close to the results of numerical simulations and observations, but it is derived from a pure probabilistic model, which may have underlying reasons worth pondering.

Xin-Xu Wang, Bao-Hua Sun, Toshitaka Kajino, Zhen-Yu He, Toshio Suzuki, Dong-Liang Fang, Zhong-Ming Niu

The $\beta^{-}$-decay rate of $^{63}$Ni, an important branching point, affects the subsequent nucleosynthesis in the weak component of the slow-neutron capture process (weak $s$-process). To evaluate the impact of the uncertainties of stellar lifetime of $^{63}$Ni on abundances, we calculate the contribution to $\beta^{-}$-decay rates from its excited states using the large-scale shell model with various interactions and also explore the atomic effects in the highly ionized plasma. In the core He burning stage and the shell C burning stage of massive stars, our new rates can be larger than those from Takahashi and Yokoi(1987) by up to a factor of 4 and 6, respectively. We evaluate the impact of the stellar decay rates of $^{63}$Ni on the nucleosynthesis of $A=60\sim90$ in a star with an initial mass of 25 $M_{\bigodot}$ and solar metalicity. We find that the new rates can lead to the abundance changes of $^{64}$Ni, $^{63}$Cu, $^{65}$Cu, $^{64}$Zn, $^{66}$Zn, $^{67}$Zn, and $^{68}$Zn by up to $18\%$, $14\%$, $7\%$, $98\%$, $16\%$, $15\%$, and $13\%$, respectively, after the shell C burning stage at the Lagrangian mass coordinate $M_{r}=2M_{\bigodot}$. The enhancement of the decay rate of $^{63}$Ni increases the weak $s$-process efficiency of nuclei after $^{65}$Cu.

Fast Radio Bursts (FRBs) are short, intense radio signals from distant astrophysical sources, and their accurate localisation is crucial for probing their origins and utilising them as cosmological tools. This study focuses on improving the astrometric precision of FRBs discovered by the Australian Square Kilometre Array Pathfinder (ASKAP) by correcting systematic positional errors in the Rapid ASKAP Continuum Survey (RACS), which is used as a primary reference for ASKAP FRB localisation. We present a detailed methodology for refining astrometry in two RACS epochs (RACS-Low1 and RACS-Low3) through crossmatching with the Wide-field Infrared Survey Explorer (WISE) catalogue. The uncorrected RACS-Low1 and RACS-Low3 catalogues had significant astrometric offsets, with all-sky median values of $0.58''$ in RA and $-0.26''$ in Dec. (RACS-Low1) and $0.29''$ in RA and $1.24''$ in Dec. (RACS-Low3), with a substantial and direction-dependent scatter around these values. After correction, the median offset was completely eliminated, and the 68\% confidence interval in the all-sky residuals was reduced to $0.2''$ or better for both surveys. By validating the corrected catalogues against other, independent radio surveys, we conclude that the individual corrected RACS source positions are accurate to a 1-$\sigma$ confidence level of $0.3''$ over the bulk of the survey area, degrading slightly to $0.4''$ near the Galactic plane. This work lays the groundwork to extend our corrections to the full RACS catalogue that will enhance future radio observations, particularly for FRB studies.

Bumhoo Lim, Masateru Ishiguro, Jun Takahashi, Hiroshi Akitakya, Jooyeon Geem, Yoonsoo P. Bach, Sunho Jin, Hangbin Jo, Seungwon Choi, Jinguk Seo, Koji S. Kawabata, Tomoya Hori, Tetsuharu Maruta, Myungshin Im

We conducted contemporaneous optical and near-infrared polarimetric and spectroscopic observations of C/2023 A3 (Tsuchinshan-ATLAS, hereafter T-A) from 2024 October 16 to December 17, covering a wide range of phase angles (20-123 deg) and wavelength (0.5-2.3 um). We paid special attention to gas contamination in the dust polarization using these data. As a result, we find the maximum polarization degree $P_max=31.21 +- 0.05 %, 33.52 +- 0.06 %, 35.12 +- 0.01 %, 37.57 +- 0.01 %, and 35.35 +- 0.01 % in the Rc-, Ic-, J-, H-, and Ks-bands, respectively. Although dust polarization shows a red slope at shorter wavelengths and can peak around 1.6 um, the phase angle at which maximum polarization occurs exhibits less dependence on wavelength (alpha_max ~ 90 deg - 95 deg). Although only a few historically bright comets, such as West, Halley, and Hale-Bopp, have undergone such extensive dust-polarization observations, our measurements are generally consistent with those of two comets that possibly originated from the Oort Cloud (West and Halley). From these results, we conjecture that the optical properties and growth processes of dust in the presolar nebula, which formed these cometary nuclei, were likely uniform.

We report the results of a spatially compete, high-sensitivity survey for Herbig-Haro (HH) outflows in the Western and Eastern Circinus molecular clouds. We have detected 28 new HH objects in Circinus West, doubling the number known in this dark nebula. We have also discovered 9 outflows in Circinus East, the first to be identified here. Although both Circinus West and East appear to be located at ~800 pc, their morphologies are distinct. Circinus West shows filamentary structure, while Circinus East is dominated by amorphous dark clouds. North-east of Circinus East, an extended distribution of young stars is centered on the ~6 Myr-old open cluster ASCC 79, which may have triggered the sequential formation of younger surrounding populations. New transverse velocities from Gaia show two dynamically distinct stellar populations in Circinus East; their velocity distribution is consistent with an active cloud-cloud collision between material ejected by the formation of O and B stars in ASCC~79 and a dynamically similar interloping cloud. Given the similar distances to Circinus West and East, and the presence in both of HH objects -- a phenomenon associated with stellar ages of ~1 Myr -- it is likely that these clouds are nominally related, but only Circinus East is subject to substantial feedback from the central cluster in the parent complex. This feedback appears to guide the morphology and evolution of Circinus East, resulting in a complex and possibly disruptive dynamical environment rich in star formation potential that contrasts with the relatively quiescent environment in Circinus West.

Recent cosmological measurements suggest the possibility of an anisotropic universe. As a result, the Bianchi Type I model, being the simplest anisotropic extension to the standard Friedmann-Lemaître-Robertson-Walker metric has been extensively studied. In this work, we show how the recombination history should be modified in an anisotropic universe and derive observables by considering the null geodesic. We then constrain the axially symmetric Bianchi Type I model by performing Markov Chain Monte Carlo with the acoustic scales in Cosmic Microwave Background (CMB) and Baryon Acoustic Oscillation data, together with local measurements of $H(z)$ and Pantheon Supernova data. Our results reveal that the anisotropic model is not worth a bare mention compared to the $\Lambda$CDM model, and we obtain a tight constraint on the anisotropy that generally agrees with previous studies under a maximum temperature anisotropy fraction of $2\times 10^{-5}$. To allow for a non-kinematic CMB dipole, we also present constraints based on a relaxed maximum temperature anisotropy comparable to that of the CMB dipole. We stress that there is a significant difference between the geodesic-based observables and the naive isotropic analogies when there is a noticeable anisotropy. However, the changes in recombination history are insignificant even under the relaxed anisotropy limit.

In 2019, the classical nova V1047 Cen experienced an unusual outburst, the nature of which has not yet been clearly determined. In this paper, we show that the 2019 V1047~Cen outburst is of Z And-type -- a type that is characteristic and has so far been observed only in symbiotic binaries. We support our claim by modeling the near-ultraviolet to near-infrared spectral energy distribution, which revealed a close similarity between the fundamental parameters and the mass-loss rate of the burning white dwarf during the 2019 V1047 Cen outburst and those measured during Z And-type outbursts in symbiotic stars. All parameters are in agreement with the theoretical prediction when the accretion rate exceeds the stable burning limit for white dwarfs with masses less than 0.7 solar units. Our analysis showed that after a nova explosion, the Z And-type outburst can occur not only in symbiotic binaries but also in short-period cataclysmic variables, when the accretion-powered system changes to a nuclear-powered one, as a consequence of the donor's reaction to the nova explosion. Such a development promotes the production of Type Ia supernovae.

Chris S. Hanson, Vivek Menon, Shravan Hanasoge, Katepalli R. Sreenivasan

Solar inertial modes have the potential to surpass the diagnostic capabilities of acoustic waves in probing the deep interior of the Sun. The fulfillment of this potential requires an accurate identification and characterization of these modes. Among the set of detected inertial modes, the equatorially anti-symmetric "high-frequency retrograde'' (HFR) modes has attracted special interest because numerical studies have suggested that they are not purely toroidal, as initial observations suggested, and predicted that they would possess a significant radial flow signal at depth. Here, we analyze $\sim$13 years of HMI/SDO 5$^\circ$ ring tiles, and discover a horizontal-divergence signal, directly connected to radial flows, in the near surface layers of the Sun. We demonstrate that this signal is indeed part of the HFR modes and not spatial leakage from prograde flows associated with magnetic regions. The amplitudes of the horizontal divergence are approximately half that associated with radial vorticity. We also report the presence of a ridge of enhanced power, although with a signal-to-noise ratio of 0.3, in the retrograde frequencies that coincides with the HFR latitudinal overtones reported by models. Using numerical linear models we find reasonable agreement with observations, though future work on boundary considerations and the inclusion of the near-surface may improve future inferences. This is the first instance where numerical studies of solar inertial modes have guided observations, giving further confidence to past inferences that rely upon numerical models.

In gamma-ray astronomy and cosmic-ray physics, the continuous approximation of inverse Compton scattering (ICS) is widely adopted to model the evolution of electron energy. However, when the initial electron energy approaches $\sim100$ TeV, the discrete nature of ICS becomes prominent, and the energy of evolved electrons should be considered as a broad distribution rather than a deterministic value. By simulating the evolution paths of individual electrons under ICS, we capture this discrete nature and demonstrate that when the electron injection spectrum exhibits a high-energy cutoff, the correct discrete treatment yields a higher cutoff energy in the evolved spectrum compared to the continuous approximation. Applying the discrete ICS treatment to interpret the gamma-ray spectrum of the Geminga pulsar halo measured by HAWC, we find that the inferred cutoff energy of the injection spectrum is correspondingly lower than that derived using the continuous approximation at a $95\%$ confidence level. This suggests that the systematic bias introduced by the approximation has exceeded the measurement precision. We also expect the application of the discrete ICS correction in the PeV regime using the ultra-high-energy gamma-ray source 1LHAASO J1954+2836u as a case study, pointing out that adopting the continuous approximation may considerably overestimate the electron acceleration capability of the source.

A.Karska, M. Figueira, A. Mirocha, M. Kaźmierczak-Barthel, Ch. Fischer, H. Wiesemeyer, I.-M. Skretas, A. Beck, S. Khan, N. Le, Y.-L. Yang, L. Looney, A. Krabbe, F. Wyrowski, K. Menten

Massive star formation is associated with energetic processes that may influence the physics and chemistry of parental molecular clouds and impact galaxy evolution. The high-mass protostar DR21 Main in Cygnus X possesses one of the largest and most luminous outflows ever detected in the Galaxy, but the origin of its structure and driving mechanisms is still debated. Our aim is to spatially resolve the far-infrared line emission from DR21 Main and to investigate the gas physical conditions, energetics, and current mass loss rates along its outflow. Far-infrared SOFIA FIFI-LS spectra covering selected high-J CO lines, OH, [O I], [CII] and [O III] lines are analyzed across the almost full extent of the DR21 Main outflow using 2.00' x 3.75' mosaic. The spatial extent of far-infrared emission follows closely the well-known outflow direction of DR21 Main in case of high-J CO, [O I] 63.18 um, and the OH line at 163.13 um. On the contrary, the emission from the [C II] 157.74 um and [O I] 145.53 um lines arises mostly from the eastern part of the outflow, and it is likely linked with a photodissociation region. Comparison of non-LTE radiative transfer models with the observed [O I] line ratios suggest H2 densities of ~10^5 cm^(-3) in the western part of the outflow and ~10^4 cm^(-3) in the East. Such densities are consistent with the predictions of UV-irradiated non-dissociative shock models for the observed ratios of CO and [O I] along the DR21 Main. Main outflow. Assuming that the bulk of emission arises in shocks, the outflow power of DR21 Main of 4.3-4.8x10^2 Lsol and the mass-loss rate of 3.3-3.7x10^(-3) Msol/yr are determined. Observations provide strong support for its origin in outflow shocks, and the stratification of physical conditions along the outflow. The total line cooling provides additional evidence that DR21 Main drives one of the most energetic outflows in the Milky Way.

Gravitational lensing of gravitational waves provides a powerful probe of the mass density distribution in the universe. Wave optics effects, such as diffraction, make the lensing effect sensitive to the structure around the Fresnel scale, which depends on the gravitational wave frequency and is typically sub-Galactic for realistic observations. Contrary to this common lore, we show that wave optics can, in principle, probe matter perturbations even below the Fresnel scale. This is achieved by introducing a new quantity derived from the amplification factor, which characterizes the lensing effect, and analyzing its correlation function. Our results demonstrate that this quantity defines an effective Fresnel scale: a characteristic scale that can be arbitrarily small, even when observational frequencies are bounded. In practice, the effective Fresnel scale is constrained by the observation time $T$ and is suppressed by a factor of $1/\sqrt{fT}$ relative to the standard Fresnel scale at frequency $f$. Nevertheless, it remains significantly smaller than the conventional Fresnel scale for $fT \gg 1$; for instance, in one-year observations of mHz GWs, the effective Fresnel scale can be as small as 1 pc. This approach opens new avenues for probing the fine-scale structure of the universe and the nature of dark matter.

Sam Taziaux, Ancla Müller, Björn Adebahr, Aritra Basu, Christoph Pfrommer, Michael Stein, Krysztof T. Chyży, Dominik J. Bomans, Torsten Enßlin, Volker Heesen, Peter Kamphuis, Marian Soida, Marek Wezgowiec, Ralf-Jürgen Dettmar, Samata Das, Julia Tjus

The study of radio emission in starburst dwarf galaxies provides a unique opportunity to investigate the mechanisms responsible for the amplification and transport of magnetic fields. Local dwarfs are often considered proxies for early-Universe galaxies, so this study may provide insights into the role of non-thermal components in the formation and evolution of larger galaxies. By investigating the radio continuum spectra and maps of the starburst dwarf galaxies, we aim to draw conclusions on their magnetic field strengths and configurations, as well as the dynamics of cosmic ray (CR) transport. We perform a radio continuum polarimetry study of two of the brightest starburst IRAS Revised Bright Galaxy Sample (RBGS) dwarf galaxies, NGC 3125 and IC 4662. By combining data of the Australian Telescope Compact Array (2.1 GHz) and MeerKAT (1.28 GHz), we analyse the underlying emission mechanism and the CR transport in these systems. We find flat spectra in those dwarf galaxies over the entire investigated frequency range, which sharply contrasts with observations of massive spiral galaxies. Because the expected cooling time of CR electrons is much shorter than their escape time, we would expect a steepened steady-state CR electron spectrum. The flat observed spectra suggest a substantial contribution from free-free emission at high frequencies and absorption at low frequencies, which may solve this puzzle. For NGC 3125, we measure a degree of polarisation between 0.75% and 2.6%, implying a turbulent field and supporting the picture of a comparably large thermal emission component that could be sourced by stellar radiation feedback and supernovae.

K. Minker, B. Carry, F. Vachier, P. Scheirich, P. Pravec, T. Müller, A. Moór, C. Arcidiacono, A. Conrad, C. Veillet, S. A. Jacobson, M. Marsset, W. J. Merline, P. Tamblyn, M. E. Brown, D. Pray, R. Montaigut, A. Leroy, C. Gillier, P. Kušnirák, K. Hornoch, M. Husárik, V. Benishek, W. Cooney, J. Gross, D. Terrell, E. Jehin, J. Világi, Š. Gajdoš, V. Chiorny, B. Christmann, J. Brinsfield, C. Dumas, B. L. Enke, D. D. Durda, J. C. Christou, W. M. Grundy, L. M. Close, S. B. Porter

The very wide binary asteroid (VWBA) population is a small subset of the population of known binary and multiple asteroids made of systems with very widely orbiting satellites and long orbital periods, on the order of tens to hundreds of days. The origin of these systems is debatable, and most members of this population are poorly characterized. We have compiled all available high-angular resolution imaging archival data of VWBA systems from large ground- and space-based telescopes. We measure the astrometric positions of the satellite relative to the primary and analyze the dynamics of the satellites using the Genoid genetic algorithm. Additionally, we use a NEATM thermal model to estimate the diameters of two systems, and we model the orbit of Litva's inner satellite using photometric lightcurve observations. We determine the effective diameters of binary systems Christophedumas and Alconrad to be 4.7 + 0.4km and 5.2 + 0.3km respectively. We determine new orbital solutions for five systems, Huenna, Litva, (3548) Eurybates, Pauling, and Alconrad. We find a significantly eccentric best-fit orbital solution for the outer satellite of Litva, a moderately eccentric solution for Alconrad, and a nearly circular solution for Pauling. We also confirm previously reported orbital solutions for (379) Huenna and Eurybates. It is unlikely that BYORP expansion could be solely responsible for the formation of VWBAs. It is possible that the satellites of these systems were formed through YORP spin-up and then later scattered onto very wide orbits. Additionally, we find that some members of the population are unlikely to have formed satellites through YORP spin-up, and a collisional formation history is favored. In particular, this applies to VWBAs within large dynamical families, or large VWBA systems such as Huenna and NASA's Lucy mission target Eurybates.

The discovery of the kilonova (KN) AT 2017gfo, accompanying the gravitational wave event GW170817, provides crucial insight into the synthesis of heavy elements during binary neutron star (BNS) mergers. Following this landmark event, another KN was detected in association with the second-brightest gamma-ray burst (GRB) observed to date, GRB 230307A, and subsequently confirmed by observations of the James Webb Space Telescope (JWST). In this work, we conduct an end-to-end simulation to analyze the temporal evolution of the KN AT 2023vfi associated with GRB 230307A, and constrain the abundances of superheavy elements produced. We find that the temporal evolution of AT 2023vfi is similar to AT 2017gfo in the first week post-burst. Additionally, the \textit{r}-process nuclide abundances of lanthanide-rich ejecta, derived from numerical relativity simulations of BNS mergers, can also successfully interpret the temporal evolution of the KN with the lanthanide-rich ejecta mass of $0.02 M_\odot$, which is consistent with the mass range of dynamical ejecta from numerical simulations in literature. Both findings strongly suggest the hypothesis that GRB 230307A originated from a BNS merger, similar to AT 2017gfo. Based on the first time observation of the KN for JWST, we are able to constrain the superheavy elements of another KN following AT 2017gfo. The pre-radioactive-decay abundances of the superheavy nuclides: $^{222}$Rn, $^{223}$Ra, $^{224}$Ra and $^{225}$Ac, are estimated to be at least on the order of $1 \times 10^{-5}$. These abundance estimates provide valuable insight into the synthesis of superheavy elements in BNS mergers, contributing to our understanding of astrophysical \textit{r}-process nucleosynthesis.

Damped Lyman-$\alpha$ absorbers (DLAs) with molecular hydrogen have been probed in detail through both spectroscopic observations and numerical modelling. However, such H$_2$ absorbers are quite sparse at very high redshifts. We identify six of the most distant known H$_2$-DLAs (redshift between 3 and 4.5), with medium/high-resolution spectroscopic observations reported in the literature, and perform detailed numerical modelling followed by Bayesian analysis to constrain their physical properties mainly using the H$_2$ rotational level population and CI fine structure levels. Our modelling approach involves setting up a constant-pressure multiphase cloud irradiated from both sides, in comparison to most models which employ constant density. This enables us to use all observed atomic and molecular species as constraints to build a more realistic model of the DLA. Our results indicate high interstellar radiation field strength $\sim$ 10$^2$ to 10$^3$ G$_0$ for some sightlines, which is suggestive of in situ star formation. The cosmic ray ionization rate for all DLAs is constrained between 10$^{-17}$ and 10$^{-14}$ s$^{-1}$, consistent with recent estimates for high-redshift sightlines. Total hydrogen density and temperature lie in the ranges 50 to 4 $\times$ 10$^4$ cm$^{-3}$ and 35-200 K in the innermost part of the absorbers. The corresponding gas pressure in our DLA models lies between 10$^{3.5}$ and 10$^{6.4}$ cm$^{-3}$ K, with three sightlines having a higher pressure than the range typical of high-redshift H$_2$-DLAs.

Existing methods for obtaining flat field rely on observed data collected under specific observation conditions to determine the flat field. However, the telescope pointing and the column fixed pattern noise of the CMOS detector change during actual observations. These leads to the residual signals in real-time observation data after flat field correction, such as interference fringes and column-fixed pattern noise. In actual observations, the wind causes the telescope to wobble slightly, which leads to shifts in the observed data. In this paper, a method of extracting the flat field from the real-time solar observation data is proposed. Firstly, the average flat field obtained by multi-frame averaging is used as the initial value. A set of real-time observation data is input into the KLL method to calculate the correction amount for the average flat field. Secondly, the average flat field is corrected using the calculated correction amount to obtain the real flat field for the current observation conditions. To overcome the residual solar structures caused by atmospheric turbulence in the correction amount, real-time observation data are grouped to calculate the correction amounts. These residual solar structures are suppressed by averaging multiple groups, improving the accuracy of the correction amount. The test results from diffraction-limited and ground-based simulated data demonstrate that our method can effectively calculate the correction amount for the average flat field. The NVST He I 10830 A/Ha data were also tested. High-resolution reconstruction confirms that the correction amount effectively corrects the average flat field to obtain the real flat field for the current observation conditions. Our method works for chromosphere and photosphere data.

Fridolin Spitzer, Christoph Burkhardt, Thomas S. Kruijer, Thorsten Kleine

Isotope anomalies in meteorites reveal a fundamental dichotomy between non-carbonaceous- (NC) and carbonaceous-type (CC) planetary bodies. Until now, this dichotomy is established for the major meteorite groups, representing about 36 distinct parent bodies. Ungrouped meteorites represent an even larger number of additional and so far mostly unexplored parent bodies. Here, the genetics and chronology of 26 ungrouped iron meteorites are investigated. The ungrouped irons confirm the NC-CC dichotomy for Mo, where NC and CC meteorites define two distinct, subparallel s-process mixing lines. All ungrouped NC irons fall on the NC-line, which is now precisely defined for 41 distinct parent bodies. The ungrouped CC irons show scatter around the CC-line indicative of small r-process Mo heterogeneities among these samples. These r-process Mo isotope variations correlate with O isotope anomalies, most likely reflecting mixing of CI chondrite-like matrix, chondrule precursors and Ca-Al-rich inclusions. This implies that CC iron meteorite parent bodies accreted the same nebular components as the later-formed carbonaceous chondrites. The Hf-W model ages of core formation for the ungrouped irons reveal a narrow age peak at ~3.3 Ma after Ca-Al-rich inclusions for the CC irons. By contrast, the NC irons display more variable ages, including younger ages indicative of impact-induced melting events, which seem absent among the CC irons. This is attributed to the more fragile and porous nature of the CC bodies, making impact-induced melting on their surfaces difficult. The chemical characteristics of all iron meteorites together reveal slightly more oxidizing conditions during core formation for CC compared to NC irons. More strikingly, strong depletions in moderately volatile elements, typical of many iron meteorite parent bodies, predominantly occur among CC irons.

Anatolii I. Visser-Zadvornyi (Kapteyn Institute), Mary E. Carstairs (Durham-ICC), Kyle A. Oman (Durham-ICC), Marc A. W. Verheijen (Kapteyn Institute)

Observational measurements hint at a peak in the quenching timescale of satellite galaxies in groups and clusters as a function of their stellar masses at $M_{\star} \approx 10^{9.5} \mathrm{M}_{\odot}$; less and more massive satellite galaxies quench faster. We investigate the origin of these trends using the EAGLE simulation in which they are qualitatively reproduced for satellites with $10^{9}<M_{\star}/\mathrm{M}_\odot<10^{11}$ around hosts of $10^{13}<M_\mathrm{200c}/\mathrm{M}_\odot<10^{14.6}$. We select gas particles of simulated galaxies at the time that they become satellites and track their evolution. Interpreting these data yields insights into the prevailing mechanism that leads to the depletion of the interstellar medium (ISM) and the cessation of star formation. We find that for satellites across our entire range in stellar mass the quenching timescale is to leading order set by the depletion of the ISM by star formation and stellar & AGN feedback in the absence of sustained accretion of fresh gas. The turnover in the quenching timescale as a function of stellar mass is a direct consequence of the maximum in the star formation efficiency (or equivalently the minimum in the total -- stellar plus AGN -- feedback efficiency) at the same stellar mass. We can discern the direct stripping of the ISM by ram pressure and/or tides in the simulations; these mechanisms modulate the quenching timescale but do not drive its overall scaling with satellite stellar mass. Our findings argue against a scenario in which the turnover in the quenching timescale is a consequence of the competing influences of gas stripping and 'starvation'.

The baryonic fraction of galaxies is observed to vary with the mass of its dark matter (DM) halo. Low-mass galaxies have low baryonic fractions which increase to a maximum for masses near $10^{12}\ M_{\odot}$, and decreases thereafter with increasing galaxy mass. This trend is generally attributed to the action of feedback from star formation at the low end and of active galactic nuclei at the high-mass end. An alternative is that the baryonic fraction is at least partially due to the ability of galaxies to competitively accrete gas in a group or clustered environment. Most galaxies in a group including those of lower masses, orbit the cluster centre at significant speeds and hence their accretion is limited by a Bondi-Hoyle type process, $\dot{M}_{acc} \propto M_{DM}^2$. In contrast, the few high-mass galaxies reside in the core of the cluster and accrete in a tidal accretion process, $\dot{M}_{acc} \propto M_{DM}^{2/3}$. These two mechanisms result in a baryonic mass fraction that increases as $M_{DM}$ at low masses and decreases as $M_{DM}^{-1/3}$ at high masses. This model predicts that lower-mass halos in small-N groups should have higher baryonic fractions relative to those in large clusters.

Andrea Costantini, Laura Iacconi, David J. Mulryne

A key step in the comparison between inflationary predictions and cosmological observations is the computation of primordial correlators. Numerical methods have been developed that overcome some of the difficulties arising in analytical calculations when the models considered are complex. The PyTransport package, which implements the transport formalism, allows computation of the tree-level 2- and 3-point correlation functions for multi-field models with arbitrary potentials and a curved field space. In this work we investigate an alternative numerical implementation of the transport approach, based on the use of transfer ''matrices'' called multi-point propagators (MPP). We test the novel MPP method, and extensively compare it with the traditional implementation of the transport approach provided in PyTransport. We highlight advantages of the former, discussing its performance in terms of accuracy, precision and running time, as well as dependence on the number of e-folds of sub-horizon evolution and tolerance settings. For topical ultra-slow-roll models of inflation we show that MPPs (i) precisely track the decay of correlators even when PyTransport produces erroneous results, (ii) extend the computation of squeezed bispectra for squeezing values at least one decade beyond those attainable with PyTransport.

Spandan Dash, Matteo Brogi, Fabian Lukas Seidler, Paolo A. Sossi, Siddharth Gandhi, Vatsal Panwar, Marina Lafarga, Peter J. Wheatley

Ultra-short Period exoplanets (USPs) like 55 Cnc e, hosting dayside magma oceans, present unique opportunities to study surface-atmosphere interactions. The composition of a vaporised mineral atmosphere enveloping the dayside is dictated by that of the surface magma ocean, which in turn is sensitive to its oxygen fugacity ($f$O$_2$). Observability estimations and characterisation of the atmospheric emission of 55 Cnc e have mostly remained limited to low spectral resolution space-based studies. Here, we aim to examine ground-based high-resolution observabilities of a diverse set of mineral atmospheres produced across a grid of mantle $f$O$_2$s varying over 12 orders of magnitude. We assume a Bulk Silicate Earth mantle composition and a substellar dayside temperature of T = 2500K in the near infrared wavelength (NIR) region. This spectral range is often featureless for this class of atmospheres at low-resolution. Coupling our newly developed simulator for synthesising realistic observations from high-resolution ground-based spectrographs (Ratri) to a pre-developed high-resolution cross-correlation spectroscopy (HRCCS) analysis pipeline (Upamana), we find that this array of mineral atmospheres would all be detectable with 11 hours of observing time of the dayside of 55 Cnc e with CARMENES and each individual scenario can be correctly differentiated within 1$\sigma$. Our analysis is readily able to distinguish between a planet with an Earth-like redox state (with $f$O$_2$ $\sim$3.5 log$_{10}$ units above the iron-wüstite, IW buffer) from a Mercury-like planet ($f$O$_2$ $\sim$5 log$_{10}$ units below IW). We thus conclude that the HRCCS technique holds promise for cataloguing the diversity of redox states among the rocky exoplanetary population.

Paolo Tortora, Riccardo Lasagni Manghi, Edoardo Gramigna, Marco Zannoni, Jan-Erik Wahlund, Jan Bergman

This work presents the simulation results of the radio science experiment onboard the proposed Heavy Metal mission to the M-type asteroid (216) Kleopatra. Earth-based radiometric measurements (range and range-rate), complemented by images from the onboard optical camera and by measurements from the inter-satellite link between the maincraft and a secondary subcraft, are used in an orbit determination process to assess the attainable accuracy for the mass of Kleopatra and its extended gravity field. Preliminary results indicate that the asteroid mass can be retrieved with a relative accuracy up to $10^{-7}$, while the extended gravity field can be estimated up to degree 10 with sufficient accuracy to discriminate between internal structure models, satisfying the scientific goals of the mission.

Matías Montesinos, Juan Garrido-Deutelmoser, Jorge Cuadra, Mario Sucerquia, Nicolás Cuello, Matthias R. Schreiber, María Paula Ronco, Octavio M. Guilera

Planetary growth within protoplanetary disks involves accreting material from their surroundings, yet the underlying mechanisms and physical conditions of the accreting gas remain debated. This study aims to investigate the dynamics and thermodynamic properties of accreting gas giants, and to characterize the envelope that forms near the planet during accretion. We employ three-dimensional hydrodynamical simulations of a Jupiter-mass planet embedded in a viscous gaseous disk. Our models incorporate a non-isothermal energy equation to compute gas and radiation energy diffusion and include radiative feedback from the planet. Results indicate that gas accretion occurs supersonically towards the planet, forming an ionized envelope that extends from the planetary surface up to 0.2 times the Hill radius in the no-feedback model, and up to 0.4 times the Hill radius in the feedback model. The envelope's radius, or ionization radius, acts as a boundary halting supersonic gas inflow and is pivotal for estimating accretion rates and H$\alpha$ emission luminosities. Including radiative feedback increases accretion rates, especially within the ionization radius and from areas to the right of the planet when the star is positioned to the left. The accretion luminosities calculated at the ionization radius are substantially lower than those calculated at the Hill radius, highlighting potential misinterpretations in the non-detection of H$\alpha$ emissions as indicators of ongoing planet formation.

H. Aussel (1), I. Tereno (2 and 3), M. Schirmer (4), G. Alguero (5), B. Altieri (6), E. Balbinot (7 and 8), T. de Boer (9), P. Casenove (10), P. Corcho-Caballero (7), H. Furusawa (11 and 12), J. Furusawa (11), M. J. Hudson (13 and 14 and 15), K. Jahnke (4), G. Libet (10), J. Macias-Perez (5), N. Masoumzadeh (16), J. J. Mohr (17), J. Odier (5), D. Scott (18), T. Vassallo (19 and 20), G. Verdoes Kleijn (7), A. Zacchei (20 and 21), N. Aghanim (22), A. Amara (23), S. Andreon (24), N. Auricchio (25), S. Awan (26), R. Azzollini (26), C. Baccigalupi (21 and 20 and 27 and 28), M. Baldi (29 and 25 and 30), A. Balestra (31), S. Bardelli (25), A. Basset (10), P. Battaglia (25), A. N. Belikov (7 and 32), R. Bender (16 and 19), A. Biviano (20 and 21), A. Bonchi (33), D. Bonino (34), E. Branchini (35 and 36 and 24), M. Brescia (37 and 38), J. Brinchmann (39 and 40), S. Camera (41 and 42 and 34), G. Cañas-Herrera (43 and 44 and 8), V. Capobianco (34), C. Carbone (45), V. F. Cardone (46 and 47), J. Carretero (48 and 49), S. Casas (50), F. J. Castander (51 and 52), M. Castellano (46), G. Castignani (25), S. Cavuoti (38 and 53), K. C. Chambers (9), A. Cimatti (54), C. Colodro-Conde (55), G. Congedo (56), C. J. Conselice (57), L. Conversi (58 and 6), Y. Copin (59), F. Courbin (60 and 61), H. M. Courtois (62), M. Cropper (26), J.-G. Cuby (63 and 64), A. Da Silva (2 and 65), R. da Silva (46 and 33), H. Degaudenzi (66), J. T. A. de Jong (7), G. De Lucia (20), A. M. Di Giorgio (67), J. Dinis (2 and 65), C. Dolding (26), H. Dole (22), M. Douspis (22), F. Dubath (66), C. A. J. Duncan (56 and 57), X. Dupac (6), S. Dusini (68), A. Ealet (59), S. Escoffier (69), M. Fabricius (16 and 19), M. Farina (67), R. Farinelli (25), F. Faustini (46 and 33), S. Ferriol (59), S. Fotopoulou (70), N. Fourmanoit (69), M. Frailis (20), E. Franceschi (25), P. Franzetti (45), S. Galeotta (20), K. George (19), W. Gillard (69), B. Gillis (56), C. Giocoli (25 and 30), P. Gómez-Alvarez (71 and 6), J. Gracia-Carpio (16), B. R. Granett (24), A. Grazian

this https URL paper submitted to the special A&A issue

The first Euclid Quick Data Release, Q1, comprises 63.1 sq deg of the Euclid Deep Fields (EDFs) to nominal wide-survey depth. It encompasses visible and near-infrared space-based imaging and spectroscopic data, ground-based photometry in the u, g, r, i and z bands, as well as corresponding masks. Overall, Q1 contains about 30 million objects in three areas near the ecliptic poles around the EDF-North and EDF-South, as well as the EDF-Fornax field in the constellation of the same name. The purpose of this data release -- and its associated technical papers -- is twofold. First, it is meant to inform the community of the enormous potential of the Euclid survey data, to describe what is contained in these data, and to help prepare expectations for the forthcoming first major data release DR1. Second, it enables a wide range of initial scientific projects with wide-survey Euclid data, ranging from the early Universe to the Solar System. The Q1 data were processed with early versions of the processing pipelines, which already demonstrate good performance, with numerous improvements in implementation compared to pre-launch development. In this paper, we describe the sky areas released in Q1, the observations, a top-level view of the data processing of Euclid and associated external data, the Q1 photometric masks, and how to access the data. We also give an overview of initial scientific results obtained using the Q1 data set by Euclid Consortium scientists, and conclude with important caveats when using the data. As a complementary product, Q1 also contains observations of a star-forming area in Lynd's Dark Nebula 1641 in the Orion~A Cloud, observed for technical purposes during Euclid's performance-verification phase. This is a unique target, of a type not commonly found in Euclid's nominal sky survey.

H. J. McCracken (1), K. Benson (2), C. Dolding (2), T. Flanet (1), C. Grenet (1), O. Herent (1), P. Hudelot (1), C. Laigle (1), G. Leroy (3 and 4), P. Liebing (2), R. Massey (4), S. Mottet (1), R. Nakajima (5), H. N. Nguyen-Kim (1), J. W. Nightingale (6), J. Skottfelt (7), L. C. Smith (8), F. Soldano (1), E. Vilenius (2), M. Wander (7), M. von Wietersheim-Kramsta (4 and 3), M. Akhlaghi (9), H. Aussel (10), S. Awan (2), R. Azzollini (2), A. Basset (11), G. P. Candini (2), P. Casenove (11), M. Cropper (2), H. Hoekstra (12), H. Israel (13), A. Khalil (2), K. Kuijken (12), Y. Mellier (14 and 1), L. Miller (15), S.-M. Niemi (16), M. J. Page (2), K. Paterson (17), M. Schirmer (17), N. A. Walton (8), A. Zacchei (18 and 19), J. P. L. G. Barrios (4 and 20), T. Erben (5), R. Hayes (4), J. A. Kegerreis (21 and 4), D. J. Lagattuta (3 and 4), A. Lançon (22), N. Aghanim (23), B. Altieri (24), A. Amara (25), S. Andreon (26), P. N. Appleton (27 and 28), N. Auricchio (29), C. Baccigalupi (19 and 18 and 30 and 31), M. Baldi (32 and 29 and 33), A. Balestra (34), S. Bardelli (29), P. Battaglia (29), A. N. Belikov (35 and 36), R. Bender (37 and 38), F. Bernardeau (39 and 1), A. Biviano (18 and 19), A. Bonchi (40), E. Branchini (41 and 42 and 26), M. Brescia (43 and 44), J. Brinchmann (45 and 46), S. Camera (47 and 48 and 49), G. Cañas-Herrera (16 and 50 and 12), V. Capobianco (49), C. Carbone (51), J. Carretero (52 and 53), S. Casas (54), F. J. Castander (55 and 56), M. Castellano (57), G. Castignani (29), S. Cavuoti (44 and 58), K. C. Chambers (59), A. Cimatti (60), C. Colodro-Conde (61), G. Congedo (62), C. J. Conselice (63), L. Conversi (64 and 24), Y. Copin (65), F. Courbin (66 and 67), H. M. Courtois (68), A. Da Silva (69 and 70), R. da Silva (57 and 40), H. Degaudenzi (71), G. De Lucia (18), A. M. Di Giorgio (72), J. Dinis (69 and 70), H. Dole (23), F. Dubath (71), X. Dupac (24), S. Dusini (73), A. Ealet (65), S. Escoffier (74), M. Fabricius (37 and 38), M. Farina

This paper describes the VIS Processing Function (VIS PF) of the Euclid ground segment pipeline, which processes and calibrates raw data from the VIS camera. We present the algorithms used in each processing element, along with a description of the on-orbit performance of VIS PF, based on Performance Verification (PV) and Q1 data. We demonstrate that the principal performance metrics (image quality, astrometric accuracy, photometric calibration) are within pre-launch specifications. The image-to-image photometric scatter is less than $0.8\%$, and absolute astrometric accuracy compared to Gaia is $5$ mas Image quality is stable over all Q1 images with a full width at half maximum (FWHM) of $0.\!^{\prime\prime}16$. The stacked images (combining four nominal and two short exposures) reach $I_\mathrm{E} = 25.6$ ($10\sigma$, measured as the variance of $1.\!^{\prime\prime}3$ diameter apertures). We also describe quality control metrics provided with each image, and an appendix provides a detailed description of the provided data products. The excellent quality of these images demonstrates the immense potential of Euclid VIS data for weak lensing. VIS data, covering most of the extragalactic sky, will provide a lasting high-resolution atlas of the Universe.

G. Polenta (1), M. Frailis (2), A. Alavi (3), P. N. Appleton (3 and 4), P. Awad (5), A. Bonchi (1), R. Bouwens (5), L. Bramante (6), D. Busonero (7), G. Calderone (2), F. Cogato (8 and 9), S. Conseil (10), M. Correnti (11 and 1), R. da Silva (11 and 1), I. Das (3), F. Faustini (11 and 1), Y. Fu (5 and 12), T. Gasparetto (2), W. Gillard (13), A. Grazian (14), S. Hemmati (3), J. Jacobson (3), K. Jahnke (15), B. Kubik (10), X. Liu (16), C. Macabiau (10), E. Medinaceli (9), P. W. Morris (16), K. Paterson (15), M. Radovich (14), M. Schirmer (15), A. Shulevski (17 and 12 and 18 and 19), H. I. Teplitz (4), B. Venemans (5), N. Aghanim (20), B. Altieri (21), A. Amara (22), S. Andreon (23), N. Auricchio (9), H. Aussel (24), C. Baccigalupi (25 and 2 and 26 and 27), M. Baldi (28 and 9 and 29), A. Balestra (14), S. Bardelli (9), A. Basset (30), P. Battaglia (9), A. N. Belikov (12 and 31), R. Bender (32 and 33), A. Biviano (2 and 25), E. Branchini (34 and 35 and 23), M. Brescia (36 and 37), J. Brinchmann (38 and 39), A. Caillat (40), S. Camera (41 and 42 and 7), G. Cañas-Herrera (43 and 44 and 5), V. Capobianco (7), C. Carbone (45), J. Carretero (46 and 47), S. Casas (48), F. J. Castander (49 and 50), M. Castellano (11), G. Castignani (9), S. Cavuoti (37 and 51), K. C. Chambers (52), A. Cimatti (53), C. Colodro-Conde (54), G. Congedo (55), C. J. Conselice (56), L. Conversi (57 and 21), Y. Copin (10), L. Corcione (7), A. Costille (40), F. Courbin (58 and 59), H. M. Courtois (60), A. Da Silva (61 and 62), H. Degaudenzi (63), G. De Lucia (2), A. M. Di Giorgio (64), H. Dole (20), F. Dubath (63), C. A. J. Duncan (55 and 56), X. Dupac (21), S. Dusini (65), A. Ealet (10), S. Escoffier (13), M. Fabricius (32 and 33), M. Farina (64), R. Farinelli (9), S. Ferriol (10), F. Finelli (9 and 66), S. Fotopoulou (67), N. Fourmanoit (13), E. Franceschi (9), M. Fumana (45), S. Galeotta (2), K. George (33), B. Gillis (55), C. Giocoli (9 and 29), P. Gómez-Alvarez

This paper describes the near-infrared processing function (NIR PF) that processes near-infrared images from the Near-Infrared Spectrometer and Photometer (NISP) instrument onboard the Euclid satellite. NIR PF consists of three main components: (i) a common pre-processing stage for both photometric (NIR) and spectroscopic (SIR) data to remove instrumental effects; (ii) astrometric and photometric calibration of NIR data, along with catalogue extraction; and (iii) resampling and stacking. The necessary calibration products are generated using dedicated pipelines that process observations from both the early performance verification (PV) phase in 2023 and the nominal survey operations. After outlining the pipeline's structure and algorithms, we demonstrate its application to Euclid Q1 images. For Q1, we achieve an astrometric accuracy of 9-15 mas, a relative photometric accuracy of 5 mmag, and an absolute flux calibration limited by the 1% uncertainty of the Hubble Space Telescope (HST) CALSPEC database. We characterise the point-spread function (PSF) that we find very stable across the focal plane, and we discuss current limitations of NIR PF that will be improved upon for future data releases.

The Euclid satellite is an ESA mission that was launched in July 2023. \Euclid is working in its regular observing mode with the target of observing an area of $14\,000~\text{deg}^2$ with two instruments, the Visible Camera (VIS) and the Near IR Spectrometer and Photometer (NISP) down to $I_{\rm E} = 24.5~\text{mag}$ ($10\, \sigma$) in the Euclid Wide Survey. Ground-based imaging data in the \textit{ugriz} bands complement the \Euclid data to enable photo-$z$ determination and VIS PSF modeling for week lensing analysis. Euclid investigates the distance-redshift relation and the evolution of cosmic structures by measuring shapes and redshifts of galaxies and clusters of galaxies out to $z\sim 2$. Generating the multi-wavelength catalogues from \Euclid and ground-based data is an essential part of the \Euclid data processing system. In the framework of the \Euclid Science Ground Segment (SGS), the aim of the MER Processing Function (PF) pipeline is to detect objects in the \Euclid imaging data, measure their properties, and MERge them into a single multi-wavelength catalogue. The MER PF pipeline performs source detection on both visible (VIS) and near-infrared (NIR) images and offers four different photometric measurements: Kron total flux, aperture photometry on PSF-matched images, template fitting photometry, and Sérsic fitting photometry. Furthermore, the MER PF pipeline measures a set of ancillary quantities, spanning from morphology to quality flags, to better characterise all detected sources. In this paper, we show how the MER PF pipeline is designed, detailing its main steps, and we show that the pipeline products meet the tight requirements that Euclid aims to achieve on photometric accuracy. We also present the other measurements (e.g. morphology) that are included in the OU-MER output catalogues and we list all output products coming out of the MER PF pipeline.

M. Tucci (1), S. Paltani (1), W. G. Hartley (1), F. Dubath (1), N. Morisset (1), M. Bolzonella (2), S. Fotopoulou (3), F. Tarsitano (1), C. Saulder (4 and 5), L. Pozzetti (2), A. Enia (6 and 2), Y. Kang (1), H. Degaudenzi (1), R. Saglia (5 and 4), M. Salvato (4), O. Ilbert (7), S. A. Stanford (8), W. Roster (4), F. J. Castander (9 and 10), A. Humphrey (11 and 12), H. Landt (13), M. Selwood (3), G. Stevens (3), N. Aghanim (14), B. Altieri (15), A. Amara (16), S. Andreon (17), N. Auricchio (2), H. Aussel (18), C. Baccigalupi (19 and 20 and 21 and 22), M. Baldi (6 and 2 and 23), A. Balestra (24), S. Bardelli (2), P. Battaglia (2), A. N. Belikov (25 and 26), F. Bernardeau (27 and 28), A. Biviano (20 and 19), A. Bonchi (29), E. Branchini (30 and 31 and 17), M. Brescia (32 and 33), J. Brinchmann (11 and 34), S. Camera (35 and 36 and 37), G. Cañas-Herrera (38 and 39 and 40), V. Capobianco (37), C. Carbone (41), J. Carretero (42 and 43), S. Casas (44), M. Castellano (45), G. Castignani (2), S. Cavuoti (33 and 46), K. C. Chambers (47), A. Cimatti (48), C. Colodro-Conde (49), G. Congedo (50), C. J. Conselice (51), L. Conversi (52 and 15), Y. Copin (53), F. Courbin (54 and 55), H. M. Courtois (56), M. Cropper (57), A. Da Silva (58 and 59), G. De Lucia (20), A. M. Di Giorgio (60), H. Dole (14), C. A. J. Duncan (50 and 51), X. Dupac (15), A. Ealet (53), S. Escoffier (61), M. Fabricius (4 and 5), M. Farina (60), R. Farinelli (2), S. Ferriol (53), F. Finelli (2 and 62), N. Fourmanoit (61), M. Frailis (20), E. Franceschi (2), M. Fumana (41), S. Galeotta (20), K. George (5), W. Gillard (61), B. Gillis (50), C. Giocoli (2 and 23), P. Gómez-Alvarez (63 and 15), J. Gracia-Carpio (4), B. R. Granett (17), A. Grazian (24), F. Grupp (4 and 5), S. V. H. Haugan (64), J. Hoar (15), H. Hoekstra (40), W. Holmes (65), I. M. Hook (66), F. Hormuth (67), A. Hornstrup (68 and 69), P. Hudelot (28), K. Jahnke (70), M. Jhabvala (71), B. Joachimi (72), E. Keihänen

The ESA Euclid mission will measure the photometric redshifts of billions of galaxies in order to provide an accurate 3D view of the Universe at optical and near-infrared wavelengths. Photometric redshifts are determined by the PHZ processing function on the basis of the multi-wavelength photometry of Euclid and ground-based observations. In this paper, we describe the PHZ processing used for the Euclid Quick Data Release, the output products, and their validation. The PHZ pipeline is responsible for the following main tasks: source classification into star, galaxy, and QSO classes based on photometric colours; determination of photometric redshifts and of physical properties of galaxies. The classification is able to provide a star sample with a high level of purity, a highly complete galaxy sample, and reliable probabilities of belonging to those classes. The identification of QSOs is more problematic: photometric information seems to be insufficient to accurately separate QSOs from galaxies. The performance of the pipeline in the determination of photometric redshifts has been tested using the COSMOS2020 catalogue and a large sample of spectroscopic redshifts. The results are in line with expectations: the precision of the estimates are compatible with Euclid requirements, while, as expected, a bias correction is needed to achieve the accuracy level required for the cosmological probes. Finally, the pipeline provides reliable estimates of the physical properties of galaxies, in good agreement with findings from the COSMOS2020 catalogue, except for an unrealistically large fraction of very young galaxies with very high specific star-formation rates. The application of appropriate priors is, however, sufficient to obtain reliable physical properties for those problematic objects. We present several areas for improvement for future Euclid data releases.

Y. Copin (1), M. Fumana (2), C. Mancini (2), P. N. Appleton (3 and 4), R. Chary (4 and 5), S. Conseil (1), A. L. Faisst (3), S. Hemmati (3), D. C. Masters (4), C. Scarlata (6), M. Scodeggio (2), A. Alavi (3), A. Carle (1), P. Casenove (7), T. Contini (8), I. Das (3), W. Gillard (9), G. Herzog (2), J. Jacobson (3), V. Le Brun (10), D. Maino (11 and 2 and 12), G. Setnikar (1), N. R. Stickley (13), D. Tavagnacco (14), Q. Xie (3), N. Aghanim (15), B. Altieri (16), A. Amara (17), S. Andreon (18), N. Auricchio (19), H. Aussel (20), C. Baccigalupi (21 and 14 and 22 and 23), M. Baldi (24 and 19 and 25), A. Balestra (26), S. Bardelli (19), A. Basset (7), P. Battaglia (19), A. N. Belikov (27 and 28), A. Biviano (14 and 21), A. Bonchi (29), E. Branchini (30 and 31 and 18), M. Brescia (32 and 33), J. Brinchmann (34 and 35), S. Camera (36 and 37 and 38), G. Cañas-Herrera (39 and 40 and 41), V. Capobianco (38), C. Carbone (2), J. Carretero (42 and 43), S. Casas (44), F. J. Castander (45 and 46), M. Castellano (47), G. Castignani (19), S. Cavuoti (33 and 48), K. C. Chambers (49), A. Cimatti (50), C. Colodro-Conde (51), G. Congedo (52), C. J. Conselice (53), L. Conversi (54 and 16), F. Courbin (55 and 56), H. M. Courtois (57), A. Da Silva (58 and 59), R. da Silva (47 and 29), H. Degaudenzi (60), S. de la Torre (10), G. De Lucia (14), A. M. Di Giorgio (61), H. Dole (15), F. Dubath (60), X. Dupac (16), S. Dusini (62), A. Ealet (1), S. Escoffier (9), M. Farina (61), R. Farinelli (19), S. Ferriol (1), F. Finelli (19 and 63), S. Fotopoulou (64), N. Fourmanoit (9), M. Frailis (14), E. Franceschi (19), P. Franzetti (2), S. Galeotta (14), K. George (65), B. Gillis (52), C. Giocoli (19 and 25), J. Gracia-Carpio (66), B. R. Granett (18), A. Grazian (26), F. Grupp (66 and 65), L. Guzzo (11 and 18 and 12), S. V. H. Haugan (67), J. Hoar (16), H. Hoekstra (41), W. Holmes (68), I. M. Hook (69), F. Hormuth (70), A. Hornstrup (71 and 72), P. Hudelot

The Euclid space mission aims to investigate the nature of dark energy and dark matter by mapping the large-scale structure of the Universe. A key component of Euclid's observational strategy is slitless spectroscopy, conducted using the Near Infrared Spectrometer and Photometer (NISP). This technique enables the acquisition of large-scale spectroscopic data without the need for targeted apertures, allowing precise redshift measurements for millions of galaxies. These data are essential for Euclid's core science objectives, including the study of cosmic acceleration and the evolution of galaxy clustering, as well as enabling many non-cosmological investigations. This study presents the SIR processing function (PF), which is responsible for processing slitless spectroscopic data. The objective is to generate science-grade fully-calibrated one-dimensional spectra, ensuring high-quality spectroscopic data. The processing function relies on a source catalogue generated from photometric data, effectively corrects detector effects, subtracts cross-contaminations, minimizes self-contamination, calibrates wavelength and flux, and produces reliable spectra for later scientific use. The first Quick Data Release (Q1) of Euclid's spectroscopic data provides approximately three million validated spectra for sources observed in the red-grism mode from a selected portion of the Euclid Wide Survey. We find that wavelength accuracy and measured resolving power are within requirements, thanks to the excellent optical quality of the instrument. The SIR PF represents a significant step in processing slitless spectroscopic data for the Euclid mission. As the survey progresses, continued refinements and additional features will enhance its capabilities, supporting high-precision cosmological and astrophysical measurements.

V. Le Brun (1), M. Bethermin (2), M. Moresco (3 and 4), D. Vibert (1), D. Vergani (4), C. Surace (1), G. Zamorani (4), A. Allaoui (1), T. Bedrine (1), P.-Y. Chabaud (1), G. Daste (1), F. Dufresne (1), M. Gray (1), E. Rossetti (5), Y. Copin (6), S. Conseil (6), E. Maiorano (4), Z. Mao (4), E. Palazzi (4), L. Pozzetti (4), S. Quai (3 and 4), C. Scarlata (7), M. Talia (3 and 4), H. M. Courtois (8), L. Guzzo (9 and 10 and 11), B. Kubik (6), A. M. C. Le Brun (12), J. A. Peacock (13), D. Scott (14), D. Bagot (15), A. Basset (15), P. Casenove (15), R. Gimenez (15), G. Libet (15), M. Ruffenach (15), N. Aghanim (16), B. Altieri (17), A. Amara (18), S. Andreon (10), N. Auricchio (4), H. Aussel (19), C. Baccigalupi (20 and 21 and 22 and 23), M. Baldi (5 and 4 and 24), A. Balestra (25), S. Bardelli (4), P. Battaglia (4), A. Biviano (21 and 20), A. Bonchi (26), D. Bonino (27), E. Branchini (28 and 29 and 10), M. Brescia (30 and 31), J. Brinchmann (32 and 33), A. Caillat (1), S. Camera (34 and 35 and 27), G. Cañas-Herrera (36 and 37 and 38), V. Capobianco (27), C. Carbone (39), J. Carretero (40 and 41), S. Casas (42), F. J. Castander (43 and 44), G. Castignani (4), S. Cavuoti (31 and 45), K. C. Chambers (46), A. Cimatti (47), C. Colodro-Conde (48), G. Congedo (13), C. J. Conselice (49), L. Conversi (50 and 17), A. Costille (1), F. Courbin (51 and 52), J.-G. Cuby (53 and 1), A. Da Silva (54 and 55), H. Degaudenzi (56), S. de la Torre (1), G. De Lucia (21), A. M. Di Giorgio (57), H. Dole (16), M. Douspis (16), F. Dubath (56), X. Dupac (17), S. Dusini (58), A. Ealet (6), S. Escoffier (59), M. Fabricius (60 and 61), M. Farina (57), R. Farinelli (4), F. Faustini (62 and 26), S. Ferriol (6), S. Fotopoulou (63), N. Fourmanoit (59), M. Frailis (21), E. Franceschi (4), M. Fumana (39), S. Galeotta (21), K. George (61), W. Gillard (59), B. Gillis (13), C. Giocoli (4 and 24), J. Gracia-Carpio

The SPE processing function (PF) of the \Euclid pipeline is dedicated to the automatic analysis of one-dimensional spectra to determine redshifts, line fluxes, and spectral classifications. The first \Euclid Quick Data Release (Q1) delivers these measurements for all $H_\mathrm{E}<22.5$ objects identified in the photometric survey. In this paper, we present an overview of the SPE PF algorithm and assess its performance by comparing its results with high-quality spectroscopic redshifts from the Dark Energy Spectroscopic Instrument (DESI) survey in the Euclid Deep Field North. Our findings highlight remarkable accuracy in successful redshift measurements, with a bias of less than $3 \times 10^{-5}$ in $(z_{\rm SPE}-z_{\rm DESI})/(1+z_{\rm DESI})$ and a high precision of approximately $10^{-3}$. The majority of spectra have only a single spectral feature or none at all. To avoid spurious detections, where noise features are misinterpreted as lines or lines are misidentified, it is therefore essential to apply well-defined criteria on quantities such as the redshift probability or the \ha\ flux and signal-to-noise ratio. Using a well-tuned quality selection, we achieve an 89\% redshift success rate in the target redshift range for cosmology ($0.9<z<1.8$), which is well covered by DESI for $z<1.6$. Outside this range where the \ha\ line is observable, redshift measurements are less reliable, except for sources showing specific spectral features (e.g., two bright lines or strong continuum). Ongoing refinements along the entire chain of PFs are expected to enhance both the redshift measurements and the spectral classification, allowing us to define the large and reliable sample required for cosmological analyses. Overall, the Q1 SPE results are promising, demonstrating encouraging potential for cosmology.

M. Walmsley (1 and 2), M. Huertas-Company (3 and 4 and 5 and 6), L. Quilley (7), K. L. Masters (8), S. Kruk (9), K. A. Remmelgas (9), J. J. Popp (10), E. Romelli (11), D. O'Ryan (12), H. J. Dickinson (10), C. J. Lintott (13), S. Serjeant (10), R. J. Smethurst (13), B. Simmons (14), J. Shingirai Makechemu (14), I. L. Garland (15), H. Roberts (16), K. Mantha (16), L. F. Fortson (16), T. Géron (1), W. Keel (17), E. M. Baeten (18), C. Macmillan (13), J. Bovy (1), S. Casas (19), C. De Leo (20), H. Domínguez Sánchez (21), J. Katona (22 and 23), A. Kovács (23 and 24), N. Aghanim (25), B. Altieri (9), A. Amara (26), S. Andreon (27), N. Auricchio (28), H. Aussel (29), C. Baccigalupi (30 and 11 and 31 and 32), M. Baldi (33 and 28 and 34), A. Balestra (35), S. Bardelli (28), A. Basset (36), P. Battaglia (28), R. Bender (37 and 38), A. Biviano (11 and 30), A. Bonchi (39), E. Branchini (40 and 41 and 27), M. Brescia (42 and 43), J. Brinchmann (44 and 45), S. Camera (46 and 47 and 48), G. Cañas-Herrera (49 and 50 and 51), V. Capobianco (48), C. Carbone (52), J. Carretero (53 and 54), F. J. Castander (55 and 56), M. Castellano (57), G. Castignani (28), S. Cavuoti (43 and 58), K. C. Chambers (59), A. Cimatti (60), C. Colodro-Conde (3), G. Congedo (61), C. J. Conselice (2), L. Conversi (62 and 9), Y. Copin (63), F. Courbin (64 and 65), H. M. Courtois (66), M. Cropper (67), A. Da Silva (68 and 69), H. Degaudenzi (70), G. De Lucia (11), A. M. Di Giorgio (71), C. Dolding (67), H. Dole (25), F. Dubath (70), C. A. J. Duncan (2), X. Dupac (9), S. Dusini (72), A. Ealet (63), S. Escoffier (73), M. Fabricius (37 and 38), M. Farina (71), R. Farinelli (28), F. Faustini (39 and 57), F. Finelli (28 and 74), P. Fosalba (56 and 55), S. Fotopoulou (75), M. Frailis (11), E. Franceschi (28), S. Galeotta (11), K. George (38), B. Gillis (61), C. Giocoli (28 and 34), P. Gómez-Alvarez (76 and 9), J. Gracia-Carpio (37), B. R. Granett (27), A. Grazian (35), F. Grupp (37 and 38), S. Gwyn (77), S. V. H. Haugan (78), H. Hoekstra

this https URL . Paper submitted as part of the A&A Special Issue `Euclid Quick Data Release (Q1)'. 16 pages, 15 figures, plus appendices

We present a detailed visual morphology catalogue for Euclid's Quick Release 1 (Q1). Our catalogue includes galaxy features such as bars, spiral arms, and ongoing mergers, for the 378000 bright ($\IE < 20.5$) or extended (area $\geq 700\,$pixels) galaxies in Q1. The catalogue was created by finetuning the Zoobot galaxy foundation models on annotations from an intensive one month campaign by Galaxy Zoo volunteers. Our measurements are fully automated and hence fully scaleable. This catalogue is the first 0.4% of the approximately 100 million galaxies where Euclid will ultimately resolve detailed morphology.

G. Stevens (1), S. Fotopoulou (1), M. N. Bremer (1), T. Matamoro Zatarain (1), K. Jahnke (2), B. Margalef-Bentabol (3), M. Huertas-Company (4 and 5 and 6 and 7), M. J. Smith (8 and 9), M. Walmsley (10 and 11), M. Salvato (12), M. Mezcua (13 and 14), A. Paulino-Afonso (15 and 16), M. Siudek (5 and 13), M. Talia (17 and 18), F. Ricci (19 and 20), W. Roster (12), N. Aghanim (21), B. Altieri (22), S. Andreon (23), H. Aussel (24), C. Baccigalupi (25 and 26 and 27 and 28), M. Baldi (29 and 18 and 30), S. Bardelli (18), P. Battaglia (18), A. Biviano (26 and 25), A. Bonchi (31), E. Branchini (32 and 33 and 23), M. Brescia (34 and 35), J. Brinchmann (16 and 36), S. Camera (37 and 38 and 39), G. Cañas-Herrera (40 and 41 and 42), V. Capobianco (39), C. Carbone (43), J. Carretero (44 and 45), M. Castellano (20), G. Castignani (18), S. Cavuoti (35 and 46), K. C. Chambers (47), A. Cimatti (48), C. Colodro-Conde (4), G. Congedo (49), C. J. Conselice (11), L. Conversi (50 and 22), Y. Copin (51), A. Costille (52), F. Courbin (53 and 54), H. M. Courtois (55), M. Cropper (56), A. Da Silva (57 and 58), H. Degaudenzi (59), G. De Lucia (26), C. Dolding (56), H. Dole (21), M. Douspis (21), F. Dubath (59), X. Dupac (22), S. Dusini (60), S. Escoffier (61), M. Farina (62), S. Ferriol (51), K. George (63), C. Giocoli (18 and 30), B. R. Granett (23), A. Grazian (64), F. Grupp (12 and 63), S. V. H. Haugan (65), I. M. Hook (66), F. Hormuth (67), A. Hornstrup (68 and 69), P. Hudelot (70), M. Jhabvala (71), E. Keihänen (72), S. Kermiche (61), A. Kiessling (73), M. Kilbinger (24), B. Kubik (51), M. Kümmel (63), H. Kurki-Suonio (74 and 75), Q. Le Boulc'h (76), A. M. C. Le Brun (77), D. Le Mignant (52), P. B. Lilje (65), V. Lindholm (74 and 75), I. Lloro (78), G. Mainetti (76), D. Maino (79 and 43 and 80), E. Maiorano (18), O. Marggraf (81), M. Martinelli (20 and 82), N. Martinet (52), F. Marulli (17 and 18 and 30), R. Massey (83), S. Maurogordato (84), H. J. McCracken (70), E. Medinaceli (18), S. Mei (85 and 86), M. Melchior (87), M. Meneghetti (18 and 30), E. Merlin

Light emission from galaxies exhibit diverse brightness profiles, influenced by factors such as galaxy type, structural features and interactions with other galaxies. Elliptical galaxies feature more uniform light distributions, while spiral and irregular galaxies have complex, varied light profiles due to their structural heterogeneity and star-forming activity. In addition, galaxies with an active galactic nucleus (AGN) feature intense, concentrated emission from gas accretion around supermassive black holes, superimposed on regular galactic light, while quasi-stellar objects (QSO) are the extreme case of the AGN emission dominating the galaxy. The challenge of identifying AGN and QSO has been discussed many times in the literature, often requiring multi-wavelength observations. This paper introduces a novel approach to identify AGN and QSO from a single image. Diffusion models have been recently developed in the machine-learning literature to generate realistic-looking images of everyday objects. Utilising the spatial resolving power of the Euclid VIS images, we created a diffusion model trained on one million sources, without using any source pre-selection or labels. The model learns to reconstruct light distributions of normal galaxies, since the population is dominated by them. We condition the prediction of the central light distribution by masking the central few pixels of each source and reconstruct the light according to the diffusion model. We further use this prediction to identify sources that deviate from this profile by examining the reconstruction error of the few central pixels regenerated in each source's core. Our approach, solely using VIS imaging, features high completeness compared to traditional methods of AGN and QSO selection, including optical, near-infrared, mid-infrared, and X-rays. [abridged]

M. Walmsley (1 and 2), P. Holloway (3), N. E. P. Lines (4), K. Rojas (5 and 4), T. E. Collett (4), A. Verma (3), T. Li (4), J. W. Nightingale (6), G. Despali (7 and 8 and 9), S. Schuldt (10 and 11), R. Gavazzi (12 and 13), A. Melo (14 and 15), R. B. Metcalf (7 and 8), I. T. Andika (15 and 14), L. Leuzzi (7 and 8), A. Manjón-García (16), R. Pearce-Casey (17), S. H. Vincken (5), J. Wilde (18), V. Busillo (19 and 20 and 21), C. Tortora (19), J. A. Acevedo Barroso (22), H. Dole (23), L. R. Ecker (24 and 25), J. Pearson (17), P. J. Marshall (26 and 27), A. More (28), T. Saifollahi (29), J. Gracia-Carpio (25), E. Baeten (30), C. Cornen (30), L. C. Johnson (31), C. Macmillan (3), S. Kruk (32), K. A. Remmelgas (32), B. Clément (22 and 33), H. Degaudenzi (34), F. Courbin (18 and 35), J. Bovy (1), S. Casas (36), H. Dannerbauer (37), J. M. Diego (38), K. Finner (39), A. Galan (15 and 14), C. Giocoli (8 and 9), N. B. Hogg (40), K. Jahnke (41), J. Katona (42 and 43), A. Kovács (43 and 44), C. De Leo (45), G. Mahler (46 and 47 and 48), M. Millon (49), B. C. Nagam (50 and 51), P. Nugent (52), A. Sainz de Murieta (4), C. M. O'Riordan (14), D. Sluse (46), A. Sonnenfeld (53), C. Spiniello (3), S. Serjeant (17), T. T. Thai (54), L. Ulivi (55 and 56 and 57), G. L. Walth (39), L. Weisenbach (4), M. Zumalacarregui (58), N. Aghanim (23), B. Altieri (32), A. Amara (59), S. Andreon (60), N. Auricchio (8), H. Aussel (61), C. Baccigalupi (62 and 63 and 64 and 65), M. Baldi (66 and 8 and 9), A. Balestra (67), S. Bardelli (8), P. Battaglia (8), F. Bernardeau (68 and 13), A. Biviano (63 and 62), A. Bonchi (69), D. Bonino (70), E. Branchini (71 and 72 and 60), M. Brescia (20 and 19), J. Brinchmann (73 and 74), S. Camera (75 and 76 and 70), G. Cañas-Herrera (77 and 78 and 79), V. Capobianco (70), C. Carbone (11), V. F. Cardone (80 and 81), J. Carretero (82 and 83), F. J. Castander (84 and 85), M. Castellano (80), G. Castignani (8), S. Cavuoti (19 and 21), K. C. Chambers (86), A. Cimatti (87), C. Colodro-Conde (88), G. Congedo (89), C. J. Conselice (2), L. Conversi

this https URL . Paper submitted as part of the A&A Special Issue `Euclid Quick Data Release (Q1)'. 20 pages, 11 figures, plus appendices

We present a catalogue of 497 galaxy-galaxy strong lenses in the Euclid Quick Release 1 data (63 deg$^2$). In the initial 0.45\% of Euclid's surveys, we double the total number of known lens candidates with space-based imaging. Our catalogue includes 250 grade A candidates, the vast majority of which (243) were previously unpublished. Euclid's resolution reveals rare lens configurations of scientific value including double-source-plane lenses, edge-on lenses, complete Einstein rings, and quadruply-imaged lenses. We resolve lenses with small Einstein radii ($\theta_{\rm E} < \ang{;;1}$) in large numbers for the first time. These lenses are found through an initial sweep by deep learning models, followed by Space Warps citizen scientist inspection, expert vetting, and system-by-system modelling. Our search approach scales straightforwardly to Euclid Data Release 1 and, without changes, would yield approximately 7000 high-confidence (grade A or B) lens candidates by late 2026. Further extrapolating to the complete Euclid Wide Survey implies a likely yield of over 100000 high-confidence candidates, transforming strong lensing science.

K. Rojas (1 and 2), T. E. Collett (2), J. A. Acevedo Barroso (3), J. W. Nightingale (4), D. Stern (5), L. A. Moustakas (5), S. Schuldt (6 and 7), G. Despali (8 and 9 and 10), A. Melo (11 and 12), M. Walmsley (13 and 14), D. J. Ballard (2 and 15), W. J. R. Enzi (2), T. Li (2), A. Sainz de Murieta (2), I. T. Andika (12 and 11), B. Clément (3 and 16), F. Courbin (17 and 18), L. R. Ecker (19 and 20), R. Gavazzi (21 and 22), N. Jackson (14), A. Kovács (23 and 24), P. Matavulj (1), M. Meneghetti (9 and 10), S. Serjeant (25), D. Sluse (26), C. Tortora (27), A. Verma (28), L. Marchetti (29 and 30 and 31), C. M. O'Riordan (11), K. McCarthy (5), S. H. Suyu (12 and 11), R. B. Metcalf (8 and 9), N. Aghanim (32), B. Altieri (33), A. Amara (34), S. Andreon (35), N. Auricchio (9), H. Aussel (36), C. Baccigalupi (37 and 38 and 39 and 40), M. Baldi (41 and 9 and 10), A. Balestra (42), S. Bardelli (9), P. Battaglia (9), R. Bender (20 and 19), A. Biviano (38 and 37), A. Bonchi (43), E. Branchini (44 and 45 and 35), M. Brescia (46 and 27), J. Brinchmann (47 and 48), S. Camera (49 and 50 and 51), G. Cañas-Herrera (52 and 53 and 54), V. Capobianco (51), C. Carbone (7), V. F. Cardone (55 and 56), J. Carretero (57 and 58), S. Casas (59), M. Castellano (55), G. Castignani (9), S. Cavuoti (27 and 60), K. C. Chambers (61), A. Cimatti (62), C. Colodro-Conde (63), G. Congedo (64), C. J. Conselice (14), L. Conversi (65 and 33), Y. Copin (66), H. M. Courtois (67), M. Cropper (68), A. Da Silva (69 and 70), H. Degaudenzi (71), G. De Lucia (38), A. M. Di Giorgio (72), C. Dolding (68), H. Dole (32), F. Dubath (71), X. Dupac (33), S. Escoffier (73), M. Fabricius (20 and 19), M. Farina (72), R. Farinelli (9), F. Faustini (43 and 55), S. Ferriol (66), F. Finelli (9 and 74), S. Fotopoulou (75), M. Frailis (38), E. Franceschi (9), S. Galeotta (38), K. George (19), W. Gillard (73), B. Gillis (64), C. Giocoli (9 and 10), P. Gómez-Alvarez (76 and 33), J. Gracia-Carpio (20), B. R. Granett (35), A. Grazian (42), F. Grupp (20 and 19), L. Guzzo (6 and 35 and 77), S. Gwyn (78), S. V. H. Haugan

We present a search for strong gravitational lenses in \Euclid imaging with high stellar velocity dispersion ($\sigmav>180\,\kms$) reported by SDSS and DESI. We performed expert visual inspection and classification of $11\,660$ \Euclid images. We discovered 38 grade A and 40 grade B candidate lenses, consistent with an expected sample of $\sim$32. Palomar spectroscopy confirmed 5 lens systems, while DESI spectra confirmed one, provided ambiguous results for another, and help to discard one. The \Euclid automated lens modeler modelled 53 candidates, confirming 38 as lenses, failing to model 9, and ruling out 6 grade B candidates. For the remaining 25 candidates we could not gather additional information. More importantly, our expert-classified non-lenses provide an excellent training set for machine learning lens classifiers. We create high-fidelity simulations of \Euclid lenses by painting realistic lensed sources behind the expert tagged (non-lens) luminous red galaxies. This training set is the foundation stone for the \Euclid galaxy-galaxy strong lensing discovery engine.

N. E. P. Lines (1), T. E. Collett (1), M. Walmsley (2 and 3), K. Rojas (4 and 1), T. Li (1), L. Leuzzi (5 and 6), A. Manjón-García (7), S. H. Vincken (4), J. Wilde (8), P. Holloway (9), A. Verma (9), R. B. Metcalf (5 and 6), I. T. Andika (10 and 11), A. Melo (11 and 10), M. Melchior (4), H. Domínguez Sánchez (12), A. Díaz-Sánchez (7), J. A. Acevedo Barroso (13), B. Clément (13 and 14), C. Krawczyk (1), R. Pearce-Casey (15), S. Serjeant (15), F. Courbin (8 and 16), G. Despali (5 and 6 and 17), R. Gavazzi (18 and 19), S. Schuldt (20 and 21), H. Degaudenzi (22), L. R. Ecker (23 and 24), W. J. R. Enzi (1), K. Finner (25), A. Galan (10 and 11), C. Giocoli (6 and 17), N. B. Hogg (26), K. Jahnke (27), S. Kruk (28), G. Mahler (29 and 30 and 31), A. More (32 and 33), B. C. Nagam (34 and 35), J. Pearson (15), A. Sainz de Murieta (1), C. Scarlata (34), D. Sluse (29), A. Sonnenfeld (36), C. Spiniello (9), T. T. Thai (18 and 37), C. Tortora (38), L. Ulivi (39 and 40 and 41), L. Weisenbach (1), M. Zumalacarregui (42), N. Aghanim (43), B. Altieri (28), A. Amara (44), S. Andreon (45), N. Auricchio (6), H. Aussel (46), C. Baccigalupi (47 and 48 and 49 and 50), M. Baldi (51 and 6 and 17), A. Balestra (52), S. Bardelli (6), P. Battaglia (6), R. Bender (24 and 23), F. Bernardeau (53 and 19), A. Biviano (48 and 47), A. Bonchi (54), D. Bonino (55), E. Branchini (56 and 57 and 45), M. Brescia (58 and 38), J. Brinchmann (59 and 60), S. Camera (61 and 62 and 55), G. Cañas-Herrera (63 and 64 and 65), V. Capobianco (55), C. Carbone (21), V. F. Cardone (66 and 67), J. Carretero (68 and 69), S. Casas (70), M. Castellano (66), G. Castignani (6), S. Cavuoti (38 and 71), K. C. Chambers (72), A. Cimatti (73), C. Colodro-Conde (74), G. Congedo (75), C. J. Conselice (3), L. Conversi (76 and 28), Y. Copin (77), A. Costille (18), H. M. Courtois (78), M. Cropper (79), A. Da Silva (80 and 81), G. De Lucia (48), A. M. Di Giorgio (82), C. Dolding (79), H. Dole (43), F. Dubath (22), C. A. J. Duncan (3), X. Dupac (28), S. Escoffier (83), M. Fabricius (24 and 23), M. Farina

Strong gravitational lensing has the potential to provide a powerful probe of astrophysics and cosmology, but fewer than 1000 strong lenses have been confirmed previously. With \ang{;;0.16} resolution covering a third of the sky, the \Euclid telescope will revolutionise strong lens finding, with \num{170000} lenses forecasted to be discovered amongst its 1.5 billion galaxies. We present an analysis of the performance of five machine-learning models at finding strong gravitational lenses in the quick release of \Euclid data (Q1), covering 63\,deg$^{2}$. The models are validated with citizen scientists and expert visual inspection. We focus on the best performing network: a fine-tuned version of the \texttt{Zoobot} pretrained model, originally trained to classify galaxy morphologies in heterogeneous astronomical imaging surveys. Of the one million Q1 objects that \texttt{Zoobot} was tasked to find strong lenses within, the top 1000 ranked objects contained 122 grade A lenses (almost certain lenses), and 41 grade B lenses (probable lenses). A deeper search with the five networks combined with visual inspection discovered 250 (247) grade A (B) lenses, of which 224 (182) are ranked in the top \num{20000} by \texttt{Zoobot}. When extrapolated to the full \Euclid survey, the highest ranked one million images will contain \num{75000} grade A or B strong gravitational lenses.

T. Li (1), T. E. Collett (1), M. Walmsley (2 and 3), N. E. P. Lines (1), K. Rojas (4 and 1), J. W. Nightingale (5), W. J. R. Enzi (1), L. A. Moustakas (6), C. Krawczyk (1), R. Gavazzi (7 and 8), G. Despali (9 and 10 and 11), P. Holloway (12), S. Schuldt (13 and 14), F. Courbin (15 and 16), R. B. Metcalf (9 and 10), D. J. Ballard (1 and 17), A. Verma (12), B. Clément (18 and 19), H. Degaudenzi (20), A. Melo (21 and 22), J. A. Acevedo Barroso (18), L. Leuzzi (9 and 10), A. Manjón-García (23), R. Pearce-Casey (24), D. Sluse (25), C. Tortora (26), R. Massey (27), G. Mahler (25 and 28 and 27), A. More (29 and 30), N. Aghanim (31), B. Altieri (32), A. Amara (33), S. Andreon (34), N. Auricchio (10), H. Aussel (35), C. Baccigalupi (36 and 37 and 38 and 39), M. Baldi (40 and 10 and 11), A. Balestra (41), S. Bardelli (10), P. Battaglia (10), R. Bender (42 and 43), F. Bernardeau (44 and 8), A. Biviano (37 and 36), A. Bonchi (45), E. Branchini (46 and 47 and 34), M. Brescia (48 and 26), J. Brinchmann (49 and 50), S. Camera (51 and 52 and 53), G. Cañas-Herrera (54 and 55 and 56), V. Capobianco (53), C. Carbone (14), V. F. Cardone (57 and 58), J. Carretero (59 and 60), S. Casas (61), M. Castellano (57), G. Castignani (10), S. Cavuoti (26 and 62), K. C. Chambers (63), A. Cimatti (64), C. Colodro-Conde (65), G. Congedo (66), C. J. Conselice (3), L. Conversi (67 and 32), Y. Copin (68), H. M. Courtois (69), M. Cropper (70), A. Da Silva (71 and 72), G. De Lucia (37), A. M. Di Giorgio (73), C. Dolding (70), H. Dole (31), F. Dubath (20), C. A. J. Duncan (3), X. Dupac (32), S. Escoffier (74), M. Fabricius (42 and 43), M. Farina (73), R. Farinelli (10), F. Faustini (45 and 57), S. Ferriol (68), F. Finelli (10 and 75), S. Fotopoulou (76), M. Frailis (37), E. Franceschi (10), S. Galeotta (37), K. George (43), W. Gillard (74), B. Gillis (66), C. Giocoli (10 and 11), P. Gómez-Alvarez (77 and 32), J. Gracia-Carpio (42), B. R. Granett (34), A. Grazian (41), F. Grupp (42 and 43), S. V. H. Haugan (78), H. Hoekstra (56), W. Holmes (6), I. M. Hook (79), F. Hormuth

Strong gravitational lensing systems with multiple source planes are powerful tools for probing the density profiles and dark matter substructure of the galaxies. The ratio of Einstein radii is related to the dark energy equation of state through the cosmological scaling factor $\beta$. However, galaxy-scale double-source-plane lenses (DSPLs) are extremely rare. In this paper, we report the discovery of four new galaxy-scale double-source-plane lens candidates in the Euclid Quick Release 1 (Q1) data. These systems were initially identified through a combination of machine learning lens-finding models and subsequent visual inspection from citizens and experts. We apply the widely-used {\tt LensPop} lens forecasting model to predict that the full \Euclid survey will discover 1700 DSPLs, which scales to $6 \pm 3$ DSPLs in 63 deg$^2$, the area of Q1. The number of discoveries in this work is broadly consistent with this forecast. We present lens models for each DSPL and infer their $\beta$ values. Our initial Q1 sample demonstrates the promise of \Euclid to discover such rare objects.

P. Holloway (1), A. Verma (1), M. Walmsley (2 and 3), P. J. Marshall (4 and 5), A. More (6), T. E. Collett (7), N. E. P. Lines (7), L. Leuzzi (8 and 9), A. Manjón-García (10), S. H. Vincken (11), J. Wilde (12), R. Pearce-Casey (13), I. T. Andika (14 and 15), J. A. Acevedo Barroso (16), T. Li (7), A. Melo (15 and 14), R. B. Metcalf (8 and 9), K. Rojas (11 and 7), B. Clément (16 and 17), H. Degaudenzi (18), F. Courbin (12 and 19), G. Despali (8 and 9 and 20), R. Gavazzi (21 and 22), S. Schuldt (23 and 24), B. C. Nagam (25 and 26), D. Sluse (27), C. Tortora (28), H. Domínguez Sánchez (29), K. Finner (30), A. Galan (14 and 15), C. Giocoli (9 and 20), L. Guzzo (23 and 31 and 32), N. B. Hogg (33), K. Jahnke (34), S. Kruk (35), G. Mahler (27 and 36 and 37), M. Millon (38), P. Nugent (39), J. Pearson (13), L. R. Ecker (40 and 41), A. Sainz de Murieta (7), C. Scarlata (25), S. Serjeant (13), A. Sonnenfeld (42), C. Spiniello (1), T. T. Thai (43), L. Ulivi (44 and 45 and 46), L. Weisenbach (7), M. Zumalacarregui (47), N. Aghanim (48), B. Altieri (35), A. Amara (49), S. Andreon (31), N. Auricchio (9), H. Aussel (50), C. Baccigalupi (51 and 52 and 53 and 54), M. Baldi (55 and 9 and 20), A. Balestra (56), S. Bardelli (9), P. Battaglia (9), R. Bender (41 and 40), A. Biviano (52 and 51), A. Bonchi (57), E. Branchini (58 and 59 and 31), M. Brescia (60 and 28), J. Brinchmann (61 and 62), S. Camera (63 and 64 and 65), G. Cañas-Herrera (66 and 67 and 68), V. Capobianco (65), C. Carbone (24), V. F. Cardone (69 and 70), J. Carretero (71 and 72), M. Castellano (69), G. Castignani (9), S. Cavuoti (28 and 73), K. C. Chambers (74), A. Cimatti (75), C. Colodro-Conde (76), G. Congedo (77), C. J. Conselice (3), L. Conversi (78 and 35), Y. Copin (79), H. M. Courtois (80), M. Cropper (81), A. Da Silva (82 and 83), G. De Lucia (52), A. M. Di Giorgio (84), C. Dolding (81), H. Dole (48), F. Dubath (18), C. A. J. Duncan (3), X. Dupac (35), S. Dusini (85), A. Ealet (79), S. Escoffier (86), M. Farina (84), R. Farinelli (9), F. Faustini (69 and 57), S. Ferriol

The Euclid Wide Survey (EWS) is expected to identify of order $100\,000$ galaxy-galaxy strong lenses across $14\,000$deg$^2$. The Euclid Quick Data Release (Q1) of $63.1$deg$^2$ Euclid images provides an excellent opportunity to test our lens-finding ability, and to verify the anticipated lens frequency in the EWS. Following the Q1 data release, eight machine learning networks from five teams were applied to approximately one million images. This was followed by a citizen science inspection of a subset of around $100\,000$ images, of which $65\%$ received high network scores, with the remainder randomly selected. The top scoring outputs were inspected by experts to establish confident (grade A), likely (grade B), possible (grade C), and unlikely lenses. In this paper we combine the citizen science and machine learning classifiers into an ensemble, demonstrating that a combined approach can produce a purer and more complete sample than the original individual classifiers. Using the expert-graded subset as ground truth, we find that this ensemble can provide a purity of $52\pm2\%$ (grade A/B lenses) with $50\%$ completeness (for context, due to the rarity of lenses a random classifier would have a purity of $0.05\%$). We discuss future lessons for the first major Euclid data release (DR1), where the big-data challenges will become more significant and will require analysing more than $\sim300$ million galaxies, and thus time investment of both experts and citizens must be carefully managed.

P. Bergamini (1 and 2), M. Meneghetti (2 and 3), A. Acebron (4), B. Clément (5 and 6), M. Bolzonella (2), C. Grillo (1 and 7), P. Rosati (8 and 2), D. Abriola (1), J. A. Acevedo Barroso (5), G. Angora (9 and 8), L. Bazzanini (8 and 2), R. Cabanac (10), B. C. Nagam (11 and 12), A. R. Cooray (13), G. Despali (14 and 2 and 3), G. Di Rosa (8), J. M. Diego (4), M. Fogliardi (8), A. Galan (15 and 16), R. Gavazzi (17 and 18), G. Granata (19), N. B. Hogg (20), K. Jahnke (21), L. Leuzzi (14 and 2), T. Li (19), M. Lombardi (1), G. Mahler (22 and 23 and 24), A. Manjón-García (25), R. B. Metcalf (14 and 2), M. Oguri (26 and 27), C. Olave (28), J. M. Palencia (4), J. Richard (29), K. Rojas (30 and 19), L. R. Ecker (31 and 32), C. Scarlata (11), M. Schirmer (21), S. Schuldt (1 and 7), D. Sluse (22), G. P. Smith (33 and 34), C. Tortora (9), G. Vernardos (35 and 36), G. L. Walth (37), J. Wilde (38), Y. Xie (5 and 39), M. Zumalacarregui (40), N. Aghanim (41), B. Altieri (42), A. Amara (43), L. Amendola (44), S. Andreon (45), N. Auricchio (2), H. Aussel (46), C. Baccigalupi (47 and 48 and 49 and 50), M. Baldi (28 and 2 and 3), A. Balestra (51), S. Bardelli (2), A. Basset (52), P. Battaglia (2), R. Bender (32 and 31), A. Biviano (48 and 47), A. Bonchi (53), D. Bonino (54), E. Branchini (55 and 56 and 45), M. Brescia (57 and 9), J. Brinchmann (58 and 59), A. Caillat (17), S. Camera (60 and 61 and 54), G. Cañas-Herrera (62 and 63 and 64), V. Capobianco (54), C. Carbone (7), J. Carretero (65 and 66), S. Casas (67), F. J. Castander (68 and 69), M. Castellano (70), G. Castignani (2), S. Cavuoti (9 and 71), K. C. Chambers (72), A. Cimatti (73), C. Colodro-Conde (74), G. Congedo (75), C. J. Conselice (76), L. Conversi (77 and 42), Y. Copin (78), F. Courbin (38 and 79), H. M. Courtois (80), M. Cropper (81), A. Da Silva (82 and 83), H. Degaudenzi (84), G. De Lucia (48), A. M. Di Giorgio (85), C. Dolding (81), H. Dole (41), F. Dubath (84), X. Dupac (42), S. Dusini (86), A. Ealet (78), S. Escoffier (87), M. Fabricius

We present the first catalogue of strong lensing galaxy clusters identified in the Euclid Quick Release 1 observations (covering $63.1\,\mathrm{deg^2}$). This catalogue is the result of the visual inspection of 1260 cluster fields. Each galaxy cluster was ranked with a probability, $\mathcal{P}_{\mathrm{lens}}$, based on the number and plausibility of the identified strong lensing features. Specifically, we identified 83 gravitational lenses with $\mathcal{P}_{\mathrm{lens}}>0.5$, of which 14 have $\mathcal{P}_{\mathrm{lens}}=1$, and clearly exhibiting secure strong lensing features, such as giant tangential and radial arcs, and multiple images. Considering the measured number density of lensing galaxy clusters, approximately $0.3\,\mathrm{deg}^{-2}$ for $\mathcal{P}_{\mathrm{lens}}>0.9$, we predict that \Euclid\ will likely see more than 4500 strong lensing clusters over the course of the mission. Notably, only three of the identified cluster-scale lenses had been previously observed from space. Thus, \Euclid has provided the first high-resolution imaging for the remaining $80$ galaxy cluster lenses, including those with the highest probability. The identified strong lensing features will be used for training deep-learning models for identifying gravitational arcs and multiple images automatically in \Euclid observations. This study confirms the huge potential of \Euclid for finding new strong lensing clusters, enabling exciting new discoveries on the nature of dark matter and dark energy and the study of the high-redshift Universe.

Euclid Collaboration, Nicolas Mai, Simona Mei, Cressida Cleland, Ranga-Ram Chary, James Bartlett, Gianluca Castignani, Helmut Dannerbauer, Gabriella De Lucia, Fabio Fontanot, Douglas Scott, Stefano Andreon, Sunayana Bhargava, Hervé Dole, Tanguy Dusserre, Adam Stanford, Vinh Phat Tran, John Weaver, Pierre-Alain Duc, Ilaria Risso

Euclid will detect tens of thousands of clusters and protoclusters at z>1.3. With a total coverage of 63.1deg^2, the Euclid Quick Data Release 1 (Q1) is large enough to detect tens of clusters and hundreds of protoclusters at these early epochs. The Q1 photometric redshift catalogue enables us to detect clusters out to z < 1.5; however, infrared imaging from Spitzer extends this limit to higher redshifts by using high local projected densities of Spitzer-selected galaxies as signposts for cluster and protocluster candidates. We use Spitzer imaging of the Euclid Deep Fields (EDFs) to derive densities for a sample of Spitzer-selected galaxies at redshifts z > 1.3, building Spitzer IRAC1 and IRAC2 photometric catalogues that are 95% complete at a magnitude limit of IRAC2=22.2, 22.6, and 22.8 for the EDF-S, EDF-F, and EDF-N, respectively. We apply two complementary methods to calculate galaxy densities: (1) aperture and surface density; and (2) the Nth-nearest-neighbour method. When considering a sample selected at a magnitude limit of IRAC2 < 22.2, at which all three EDFs are 95% complete, our surface density distributions are consistent among the three EDFs and with the SpUDS blank field survey. We also considered a deeper sample (IRAC2 < 22.8), finding that 2% and 3% of the surface densities in the North and Fornax fields are 3 sigma higher than the average field distribution and similar to densities found in the CARLA cluster survey. Our surface densities are also consistent with predictions from the GAEA semi-analytical model. Using combined Euclid and ground-based i-band photometry we show that our highest Spitzer-selected galaxy overdence regions, found at z~1.5, also host high densities of passive galaxies. This means that we measure densities consistent with those found in clusters and protoclusters at z>1.3.

C. Laigle (1), C. Gouin (1), F. Sarron (2 and 3), L. Quilley (4), C. Pichon (1 and 5), K. Kraljic (6), F. Durret (7), N. E. Chisari (8 and 9), U. Kuchner (10), N. Malavasi (11), M. Magliocchetti (12), H. J. McCracken (1), J. G. Sorce (13 and 14), Y. Kang (15), C. J. R. McPartland (16 and 17), S. Toft (18 and 17), N. Aghanim (14), B. Altieri (19), A. Amara (20), S. Andreon (21), N. Auricchio (22), H. Aussel (23), C. Baccigalupi (24 and 25 and 26 and 27), M. Baldi (28 and 22 and 29), A. Balestra (30), S. Bardelli (22), A. Basset (31), P. Battaglia (22), F. Bernardeau (32 and 1), A. Biviano (25 and 24), A. Bonchi (33), E. Branchini (34 and 35 and 21), M. Brescia (36 and 37), J. Brinchmann (38 and 39), S. Camera (40 and 41 and 42), G. Cañas-Herrera (43 and 44 and 9), V. Capobianco (42), C. Carbone (45), J. Carretero (46 and 47), S. Casas (48), M. Castellano (49), G. Castignani (22), S. Cavuoti (37 and 50), K. C. Chambers (51), A. Cimatti (52), C. Colodro-Conde (53), G. Congedo (54), C. J. Conselice (55), L. Conversi (56 and 19), Y. Copin (57), F. Courbin (58 and 59), H. M. Courtois (60), M. Cropper (61), A. Da Silva (62 and 63), H. Degaudenzi (15), S. de la Torre (64), G. De Lucia (25), A. M. Di Giorgio (12), C. Dolding (61), H. Dole (14), F. Dubath (15), C. A. J. Duncan (55), X. Dupac (19), A. Ealet (57), S. Escoffier (65), M. Farina (12), R. Farinelli (22), F. Faustini (33 and 49), S. Ferriol (57), F. Finelli (22 and 66), S. Fotopoulou (67), M. Frailis (25), E. Franceschi (22), S. Galeotta (25), K. George (68), W. Gillard (65), B. Gillis (54), C. Giocoli (22 and 29), P. Gómez-Alvarez (69 and 19), J. Gracia-Carpio (11), B. R. Granett (21), A. Grazian (30), F. Grupp (11 and 68), S. Gwyn (70), S. V. H. Haugan (71), H. Hoekstra (9), W. Holmes (72), I. M. Hook (73), F. Hormuth (74), A. Hornstrup (75 and 16), P. Hudelot (1), K. Jahnke (76), M. Jhabvala (77), B. Joachimi (78), E. Keihänen (79), S. Kermiche (65), A. Kiessling (72), M. Kilbinger (23), B. Kubik

Galaxy morphologies and shape orientations are expected to correlate with their large-scale environment, since they grow by accreting matter from the cosmic web and are subject to interactions with other galaxies. Cosmic filaments are extracted in projection from the Euclid Quick Data Release 1 (covering 63.1 $\mathrm{deg}^2$) at $0.5<z<0.9$ in tomographic slices of 170 comoving $h^{-1}\mathrm{Mpc}$ using photometric redshifts. Galaxy morphologies are accurately retrieved thanks to the excellent resolution of VIS data. The distribution of massive galaxies ($M_* > 10^{10} M_\odot$) in the projected cosmic web is analysed as a function of morphology measured from VIS data. Specifically, the 2D alignment of galaxy shapes with large-scale filaments is quantified as a function of Sérsic indices and masses. We find the known trend that more massive galaxies are closer to filament spines. At fixed stellar masses, morphologies correlate both with densities and distances to large-scale filaments. In addition, the large volume of this data set allows us to detect a signal indicating that there is a preferential alignment of the major axis of massive early-type galaxies along projected cosmic filaments. Overall, these results demonstrate our capabilities to carry out detailed studies of galaxy environments with Euclid, which will be extended to higher redshift and lower stellar masses with the future Euclid Deep Survey.

We use the observed vertical velocity field, of various young tracers of the gas kinematics, obtained by Li and Chen (2022), Konietzka et al. (2024) and Zhu et al. (2024), in order to test for the existence of turbulence. We do so by computing the power spectrum and the structure function of the vertical velocity field. The latter suggest the existence of compressible, Burgers, turbulence. The turbulence timescale on the largest spatial scale is about 500 Myr , implying that the turbulence has been generated 500 Myr ago. The turbulence region depth in a direction perpendicular to the Radcliffe wave direction is about 400 pc.

In the early stages of star formation, boundary layer accretion, where protostars accrete material from disks extending down to their surfaces, plays a crucial role. Understanding how a magneto-rotational-instability (MRI)-active disk connects to a protostar's surface remains a significant challenge. To investigate the mechanisms of mass and angular momentum transfer, we develop a global, three-dimensional magnetohydrodynamic model of boundary layer accretion around a magnetized, convective low-mass protostar. Our results reveal that angular momentum transport mechanisms transition significantly from the outer MRI-active disk to the protostellar surface. Various mechanisms--MRI, spiral shocks, coronal accretion, jets, and disk winds--contribute to angular momentum transfer, resulting in three distinct disk structures: (1) the MRI-active disk, (2) the transition layer, and (3) the boundary layer. The simulated protostar is strongly magnetized due to the accumulation of the disk fields, wrapping by disk toroidal fields, and stellar dynamo activity. Magnetic concentrations analogous to starspots form on the protostar and interact with the rotating disk gas to generate spiral shocks. These shocks play a key role in driving accretion. These findings demonstrate the necessity of global MHD models for a comprehensive understanding of angular momentum transport. Additionally, we identify explosive events triggered by magnetic reconnection in both the protostar and the disk atmosphere. We also find decretion flows in the disk midplane, which may be important for the radial transport of refractory materials, such as Calcium-Aluminium-rich Inclusions (CAIs) precursor gas, to the outer disk.

The observation of gravitational waves from merging black holes and neutron stars provides a unique opportunity to discern information about their astrophysical environment. Two signatures that are considered powerful tracers to distinguish between different binary formation channels are general-relativistic spin-induced orbital precession and orbital eccentricity. Both effects leave characteristic imprints in the gravitational-wave signal that can be extracted from observations. To date, neither precession nor eccentricity have been discerned in neutron star - black hole binaries. Here we report the first measurement of orbital eccentricity in a neutron star - black hole binary. Using, for the first time, a waveform model that incorporates precession and eccentricity, we perform Bayesian inference on the event GW200105 and infer a median orbital eccentricity of $e_{20}\sim 0.145$ at an orbital period of $0.1$s, excluding zero at more than $99\%$ confidence. We find inconclusive evidence for the presence of precession, consistent with previous, non-eccentric results. Our result implies a fraction of these binaries will exhibit orbital eccentricity even at small separations, suggesting formation through mechanisms involving dynamical interactions beyond isolated binary evolution. Future observations will reveal the contribution of eccentric neutron star - black hole binaries to the total merger rate across cosmic time.

Incompressible vortex flow are observed in a large variety of astrophysical plasmas such as the convection zone and the atmosphere of stars, in astrophysical jets in stellar winds and in planetary magnetospheres. More specifically, magnetohydrodynamic (MHD) simulations have shown that two large scale interlaced Alfvénic vortices structure the magnetic tail of Uranus at solstice time. Assuming identical vortices, we compute the general linear structure of the flow near their centers within the frame of ideal MHD. We then use the analytic results to interpret and qualify the vortices observed in a 3D MHD simulation of a fast rotating Uranus-type planet.

M. Pillas, S. Antier, K. Ackley, T. Ahumada, D. Akl, L. de Almeida, S. Anand, C. Andrade, I. Andreoni, K. A. Bostroem, M. Bulla, E. Burns, T. Cabrera, S. Chang, H. Choi, B. O'Connor, M. W. Coughlin, W. Corradi, A. R. Gibbs, T. Dietrich, D. Dornic, J.-G. Ducoin, P.-A. Duverne, M. Dyer, H.-B. Eggenstein, M. Freeberg, M. Fausnaugh, W. Fong, F. Foucart, D. Frostig, N. Guessoum, V. Gupta, P. Hello, G. Hosseinzadeh, L. Hu, T. Hussenot-Desenonges, M. Im, R. Jayaraman, M. Jeong, V. Karambelkar, S. Karpov, M. Kasliwal, C. D. Kilpatrick, S. Kim, N. Kochiashvili, K. Kunnumkai, M. Lamoureux, C. U. Lee, N. Lourie, J. Lyman, F. Magnani, M. Masek, G. Mo, M. Molham, F. Navarete, D. O'Neill, M. Nicholl, A. H. Nitz, K. Noysena, G. S.H. Paek, A. Palmese, R. Poggiani, T. Pradier, O. Pyshna, Y. Rajabov, J. C. Rastinejad, D. J. Sand, P. Shawhan, M. Shrestha, R. Simcoe, S. J. Smartt, D. Steeghs, R. Stein, H. F. Stevance, M. Sun, A. Takey, A. Toivonen, D. Turpin, K. Ulaczyk, A. Wold, T. Wouters

Neutron star-black hole (NSBH) mergers, detectable via their gravitational-wave (GW) emission, are expected to produce kilonovae (KNe). Four NSBH candidates have been identified and followed-up by more than fifty instruments since the start of the fourth GW Observing Run (O4), in May 2023, up to July 2024; however, no confirmed associated KN has been detected. This study evaluates ejecta properties from multi-messenger observations to understand the absence of detectable KN: we use GW public information and joint observations taken from 05.2023 to 07.2024 (LVK, ATLAS, DECam, GECKO, GOTO, GRANDMA, SAGUARO, TESS, WINTER, ZTF). First, our analysis on follow-up observation strategies shows that, on average, more than 50% of the simulated KNe associated with NSBH mergers reach their peak luminosity around one day after merger in the $g,r,i$- bands, which is not necessarily covered for each NSBH GW candidate. We also analyze the trade-off between observation efficiency and the intrinsic properties of the KN emission, to understand the impact on how these constraints affect our ability to detect the KN, and underlying ejecta properties for each GW candidate. In particular, we can only confirm the kilonova was not missed for 1% of the GW230529 and S230627c sky localization region, given the large sky localization error of GW230529 and the large distance for S230627c and, their respective KN faint luminosities. More constraining, for S230518h, we infer the dynamical ejecta and post-merger disk wind ejecta $m_{dyn}, m_{wind}$ $<$ $0.03$ $M_\odot$ and the viewing angle $\theta>25^\circ$. Similarly, the non-astrophysical origin of S240422ed is likely further confirmed by the fact that we would have detected even a faint KN at the time and presumed distance of the S240422ed event candidate, within a minimum 45% credible region of the sky area, that can be larger depending on the KN scenario.

Nelson Caldwell, John C. Raymond, Knox S.Long, Myung Gyoon Lee

With a star formation rate of order 0.4 M$_\odot $ yr$^{-1}$, M31 should have significant population of supernova remnants (SNRs), and, in fact, 156 SNR and SNR candidates have been suggested by Lee et al. (2014) by searching for nebulae with elevated [SII]/H${\alpha}$ ratios in narrow band images. Here we use a combination of low and high resolution optical spectroscopy obtained with Hectospec on the MMT to characterize 152 of these nebulae. Of these candidates, we find 93 nebulae that have [SII]/H${\alpha}$ ratios that exceed 0.4, the traditional ratio used to separate SNRs from HII regions, strongly suggesting that at least these objects are SNRs. Our high resolution spectroscopy reveals 108 nebulae that have velocity widths in H${\alpha} $ (full-width at 20% peak flux) that exceed 50 km s$^{-1}$, significantly larger than found in HII regions. There are 72 objects that satisfy both tests. Here we discuss the spectroscopic characteristics of all of the objects in our sample, and the likelihood that other objects in the sample of Lee et al. are also SNRs, and we briefly consider confirmation by X-ray, radio and UV observations. We also discuss several new candidates that have been identified serendipitously in the course of examining a large amount of archival Hectospec data.

Deep Ghuge, Debesh Bhattacharjee, Prasad Subramanian

Solar coronal mass ejections (CMEs) directed at the Earth often drive large geomagnetic storms. Here we use velocity, magnetic field and proton density data from 152 CMEs that were sampled in-situ at 1 AU by the WIND spacecraft. We Fourier analyze fluctuations of these quantities in the quiescent pre-CME solar wind, sheath and magnetic cloud. We quantify the extent by which the power in turbulent (magnetic field, velocity and density) fluctuations in the sheath exceeds that in the solar wind background and in the magnetic cloud. For instance, the mean value of the power per unit volume in magnetic field fluctuations in the sheath is 76.7 times that in the solar wind background, while the mean value of the power per unit mass in velocity fluctuations in the sheath is 9 times that in the magnetic cloud. Our detailed results show that the turbulent fluctuation power is a useful discriminator between the ambient solar wind background, sheaths and magnetic clouds and can serve as a useful input for space weather prediction.

Until the second half of the 19th century, two or more brief appearances of bright comets, such as the ones in 1668 and 1702, alike in aspect and motion, seen with a tail near the Sun, were almost universally believed to be periodic returns of a single object. It is likely that the exceptional story of Halley's comet was the compelling precedent for this school of thought. Application to sungrazers was discredited by the observed fragmentation of the nucleus of the giant sungrazer of 1882 shortly after perihelion. Generally, separations and orbital periods of the Kreutz comets are known to be governed in such events by the solar tidal force, while the range in the longitude of the nodal line is linked to the pyramidal architecture caused by nontidal, cascading fragmentation along the entire orbit and described by an updated contact-binary model. Perception of the sungrazer system was changed dramatically by coronagraphic imaging from space, which led to discovery of up to ten populations of dwarf comets. Past fragmentation patterns have been used to tentatively predict the arrivals of two bright Kreutz sungrazers -- a Population II member around 2027 (and before 2040) and a Population I member around 2050.

Joshua D. Lothringer, Katherine A. Bennett, David K. Sing, Brian Kehoe-Seamons, Zafar Rustamkulov, Henrique Reggiani, Kevin C. Schlaufman, Patrick McCreery, Seti Norris, Peter Hauschildt, Ceiligh Cacho-Negrete, Amélie Gressier, Néstor Espinoza, Cyril Gapp, Thomas M. Evans-Soma, Kevin B. Stevenson, Hannah R. Wakeford, Neale Gibson, Jamie Wilson, Nikolay Nikolov

The atmospheres of ultra-hot Jupiters are unique compared to other planets because of the presence of both refractory and volatile gaseous species, enabling a new lens to constrain a planet's composition, chemistry, and formation. WASP-178b is one such ultra-hot Jupiter that was recently found to exhibit enormous NUV absorption between 0.2 and 0.4 $\mu$m from some combination of Fe+, Mg, and SiO. Here, we present new infrared observations of WASP-178b with HST/WFC3 and JWST/NIRSpec/G395H, providing novel measurements of the volatile species H$_2$O and CO in WASP-178b's atmosphere. Atmospheric retrievals find a range of compositional interpretations depending on which dataset is retrieved, the type of chemistry assumed, and the temperature structure parametrization used due to the combined effects of thermal dissociation, the lack of volatile spectral features besides H$_2$O and CO, and the relative weakness of H$_2$O and CO themselves. Taken together with a new state-of-the-art characterization of the host star, our retrieval analyses suggests a solar to super-solar [O/H] and [Si/H], but sub-solar [C/H], perhaps suggesting rock-laden atmospheric enrichment near the H$_2$O iceline. To obtain meaningful abundance constraints for this planet, it was essential to combine the JWST IR data with short-wavelength HST observations, highlighting the ongoing synergy between the two facilities.

Klaus Paschek, Thomas K. Henning, Karan Molaverdikhani, Yoshinori Miyazaki, Ben K. D. Pearce, Ralph E. Pudritz, Dmitry A. Semenov

Understanding what environmental conditions prevailed on early Earth during the Hadean eon, and how this set the stage for the origins of life, remains a challenge. Geologic processes such as serpentinization and bombardment by chondritic material during the late veneer might have been very active, shaping an atmospheric composition reducing enough to allow efficient photochemical synthesis of HCN, one of the key precursors of prebiotic molecules. HCN can rain out and accumulate in warm little ponds (WLPs), forming prebiotic molecules such as nucleobases and the sugar ribose. These molecules could condense to nucleotides, the building blocks of RNA molecules, one of the ingredients of life. Here, we perform a systematic study of potential sources of reducing gases on Hadean Earth and calculate the concentrations of prebiotic molecules in WLPs based on a comprehensive geophysical and atmospheric model. We find that in a reduced H$_2$-dominated atmosphere, carbonaceous bombardment can produce enough HCN to reach maximum WLP concentrations of $\sim 1-10\,\mathrm{mM}$ for nucleobases and, in the absence of seepage, $\sim 10-100\,\mathrm{\mu M}$ for ribose. If the Hadean atmosphere was initially oxidized and CO$_2$-rich ($90\,\%$), we find serpentinization alone can reduce the atmosphere, resulting in WLP concentrations of an order of magnitude lower than the reducing carbonaceous bombardment case. In both cases, concentrations are sufficient for nucleotide synthesis, as shown in experimental studies. RNA could have appeared on Earth immediately after it became habitable (about $100\,\mathrm{Myr}$ after the Moon-forming impact), or it could have (re)appeared later at any time up to the beginning of the Archean.

We show that the consistent application of the rules of quantum mechanics to cosmological systems inevitably results in the so-called multiverse states in which neither the background spacetime nor the inhomogeneous perturbation are in definite states. We study the multiverse states as perturbations to the usually employed so-called Born-Oppenheimer states that are products of a wave function of the background and a wave function of the perturbation. The obtained corrections involve integrals over \emph{virtual backgrounds} that represent the effect of quantum background fluctuations on the perturbation state. They resemble loop corrections in quantum field theory. This approach demonstrates the inevitable existence of very specific non-Gaussian features in primordial fluctuations. We express the resulting non-Gaussian perturbation as a nonlinear function of the Gaussian perturbation obtained within the Born-Oppenheimer approximation, and compute its trispectrum, to show that the multiverse scenario leads to testable and distinct signatures in cosmological perturbations. Our approach applies both to inflationary and alternative cosmologies.

Similar to particle accelerators, black holes also have the ability to accelerate particles, generating significant amounts of energy through particle collisions. In this study, we examine the horizon and spacetime structures of a rotating black hole within the framework of Einstein-Maxwell-Dilaton gravity. Additionally, we extend the analysis to explore particle collisions and energy extraction near this black hole using the Banados-Silk-West mechanism. Our findings reveal that the mass and angular momentum of the colliding particles significantly influence the center of mass energy, more so than the parameters of the black hole itself. Furthermore, we apply the Banados-Silk-West mechanism to massless particles, particularly photons, while disregarding their intrinsic spin in plasma; an aspect that has not been previously explored. The Banados-Silk-West mechanism cannot be directly applied, as the refractive index condition only permits photon propagation, meaning that massive particles in vacuum cannot be included in this study. We derive the propagation conditions for photons and analyze photon collisions by treating them as massive particles in a dispersive medium. The impact of the plasma parameter on the extracted center of mass energy is also examined. Our results show that the plasma parameter has a relatively weak and unchanged effect on the center of mass energy across all cases, indicating that energy losses due to friction within the medium are a contributing factor.

K. Aggarwal, I. Arnquist, N. Avalos, X. Bertou, N. Castelló-Mor, A.E. Chavarria, J. Cuevas-Zepeda, A. Dastgheibi-Fard, C. De Dominicis, O. Deligny, J. Duarte-Campderros, E. Estrada, R. Gaïor, E.-L. Gkougkousis, T. Hossbach, L. Iddir, B. J. Kavanagh, B. Kilminster, A. Lantero-Barreda, I. Lawson, A. Letessier-Selvon, H. Lin, P. Loaiza, A. Lopez-Virto, R. Lou, K. J. McGuire, S. Munagavalasa, J. Noonan, D. Norcini, S. Paul, P. Privitera, P. Robmann, B. Roach, M. Settimo, R. Smida, M. Traina, R. Vilar, R. Yajur, D. Venegas-Vargas, C. Zhu, Y. Zhu

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We report on a search for sub-GeV dark matter (DM) particles interacting with electrons using the DAMIC-M prototype detector at the Modane Underground Laboratory. The data feature a significantly lower detector single $e^-$ rate (factor 50) compared to our previous search, while also accumulating a ten times larger exposure of $\sim$1.3 kg-day. DM interactions in the skipper charge-coupled devices (CCDs) are searched for as patterns of two or three consecutive pixels with a total charge between 2 and 4 $e^-$. We find 144 candidates of 2 $e^-$ and 1 candidate of 4 $e^-$, where 141.5 and 0.071, respectively, are expected from background. With no evidence of a DM signal, we place stringent constraints on DM particles with masses between 1 and 1000 MeV/$c^2$ interacting with electrons through an ultra-light or heavy mediator. For large ranges of DM masses below 1 GeV/c$^2$, we exclude theoretically-motivated benchmark scenarios where hidden-sector particles are produced as a major component of DM in the Universe through the freeze-in or freeze-out mechanisms.

Duarte Feiteira (1), Oleg Lebedev (1) ((1) Department of Physics and Helsinki Institute of Physics, Helsinki, Finland)

We study production of free and feebly interacting scalars during inflation using the Bogolyubov coefficient and Starobinsky stochastic approaches. While the two methods agree in the limit of infinitely long inflation, the Starobinsky approach is more suitable for studying realistic situations, where the duration of inflation is finite and the scalar field has non-trivial initial conditions. We find that the abundance of produced particles is sensitive to pre-inflationary initial conditions, resulting in the uncertainty of many orders of magnitude. Nevertheless, a lower bound on the particle abundance can be obtained. High scale inflation is very efficient in particle production, which leads to strong constraints on the existence of stable scalars with masses below the inflationary Hubble rate. For example, free stable scalars are allowed only if they have masses below an eV or the reheating temperature is in the GeV range or below. We find universal scaling behavior of the particle abundance, which covers free and feebly interacting scalars as well as those with a small non-minimal coupling to gravity. These considerations are important in the context of non-thermal dark matter since inflationary particle production provides an irreducible background for other production mechanisms.

There is no standard numerical implementation of the Hall effect, which is one of the non-ideal magnetohydrodynamic (MHD) effects. Numerical instability arises when a simple implementation is used, in which the Hall electric field is added to the electric field to update magnetic fields without further modifications to the numerical scheme. In this paper, several implementations proposed in the literature are compared to identify an approach that provides stable and accurate results. We consider two types of implementations of the Hall effect. One is a modified version of the Harten-Lax-van Leer method (Hall-HLL) in which the phase speeds of whistler waves are adopted as the signal speeds; the other involves adding a fourth-order hyper-resistivity to a Hall-MHD code. Based on an extensive series of test calculations, we found that hyper-resistivity yields more accurate results than the Hall-HLL, particularly in problems where the whisler-wave timescale is shorter than the the timescale of physical processes of interest. Through both von Neumann stability analysis and numerical experiments, an appropriate coefficient for the hyper-resistivity is determined.

John Joseph Carrasco, Renata Kallosh, Andrei Linde, Diederik Roest

The $SL(2,\mathbb{Z})$ invariant $\alpha$-attractor models have plateau potentials with respect to the inflaton and axion fields. The potential in the axion direction is almost exactly flat during inflation, hence, the axion field remains nearly massless. In this paper, we develop a generalized class of such models, where the $SL(2,\mathbb{Z})$ symmetry is preserved, but the axion acquires a large mass and becomes strongly stabilized during inflation, which eliminates isocurvature perturbations in this scenario. Inflation in such two-field models occurs as in the single-field $\alpha$-attractors and leads to the same cosmological predictions.

We discuss the fine-tunings of nuclear reactions in the Big Bang and in stars and draw some conclusions on the emergence of the light elements and the life-relevant elements carbon and oxygen. We also stress how to improve these calculations in the future. This requires a concerted effort of different communities, especially in nuclear reaction theory, lattice QCD for few-nucleon systems, stellar evolution calculations, particle physics and philosophy.

The lack of a dynamical framework within doubly special relativity theories has impeded the development of a corresponding phenomenology of modified interactions. In this work we show that in a model based on the classical basis of $\kappa$-Poincaré and total momentum conservation, one has a well-defined cross section of the photon-photon annihilation process, once a prescription for the channel treatment is set. The modification of the interaction can lead to observable effects in the opacity of the Universe to very high-energy gamma rays when the gamma-ray energy approaches the energy scale of the deformation. The magnitude and observability of this deformation are examined as functions of the gamma-ray energy and source distance.

Discovering Lorentz-invariance violation (LIV) would upend the foundations of modern physics. Because LIV effects grow with energy, high-energy astrophysical neutrinos provide the most sensitive tests of Lorentz invariance in the neutrino sector. We examine an understudied yet phenomenologically rich LIV signature: compass asymmetries, where neutrinos of different flavors propagate preferentially along different directions. Using the directional flavor composition of high-energy astrophysical neutrinos, i.e., the abundances of $\nu_{e}$, $\nu_{\mu}$, and $\nu_{\tau}$ across the sky, we find no evidence of LIV-induced flavor anisotropy in 7.5 years of IceCube High-Energy Starting Events. Thus, we place upper limits on the values of hundreds of LIV parameters with operator dimensions 2-8, tightening existing limits by orders of magnitude and bounding hundreds of parameters for the first time.