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Papers for Friday, Sep 19 2025

Papers with local authors

Gravitational effects are known to violate global symmetries, threatening the Peccei-Quinn (PQ) solution to the strong CP problem. Ultraviolet completions featuring a gauged $U(1)$ symmetry, where $U(1)_{\rm PQ}$ arises as an accidental global symmetry, can suppress Planck-suppressed operators, enabling high-quality axions in a mass window where it can also account for the observed dark matter (DM) in the Universe. We show that in such models, the spontaneous breaking of the $U(1)$ gauge symmetry generates a strong stochastic gravitational wave background (SGWB) from gauge cosmic string loops. For breaking scales $\gtrsim 10^{14}$ GeV, the SGWB signal strength exceeds astrophysical foregrounds across a broad frequency range. Contrary to conventional gauge cosmic string scenarios, such quality axion models have a characteristic IR break frequency originating from the collapse of string-wall network around axion oscillation temperature. We propose this characteristic SGWB frequency-amplitude region, identified as \textit{Signature-Window-Axion-Gravitational waves} (SWAG), to be a novel probe of high-quality axion DM at future space and ground-based interferometers.

Zhen-Ya Zheng, Chun Xu, Xiaohua Liu, Yong-He Chen, Fang Xu, Hu Zhan, Xinfeng Li, Lixin Zheng, Huanyuan Shan, Jing Zhong, Zhaojun Yan, Fang-Ting Yuan, Chunyan Jiang, Xiyan Peng, Wei Chen, Xue Cheng, Zhen-Lei Chen, Shuairu Zhu, Lin Long, Xin Zhang, Yan Gong, Li Shao, Wei Wang, Tianyi Zhang, Guohao Ju, Chenghao Li, Wei Wang, Zhiyuan Li, Tao Wang, Junfeng Wang, Chengyuan Li, Bin Ma, Jianguo Wang, Lei Wang, Dezi Liu, Nie Lin, Kexin Li, Xinrong Wen, Maochun Wu, Ruqiu Lin, Xiang Ji
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Paper 33 — arXiv:2509.14691
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Paper 33 — arXiv:2509.14691

The Multi-Channel Imager (MCI) is a powerful near-ultraviolet (NUV) and visible imager onboard the Chinese Space Station Survey Telescope (CSST). The MCI provides three imaging channels, which are the NUV channel, the Optical-blue channel and the Optical-red channel, with the wavelength range of 255-430 nm, 430-700 nm, and 700-1000 nm, respectively. The three channels can target the same field simultaneously. Each channel employs a CCD focal plane of 9216 x 9232 pixels and $\sim$7.5 x 7.5 arcmin$^2$ field of view. The MCI's three channels feature unprecedented sensitivities and field of views, as well as rich filter sets, which complements the NUV and visible capabilities of the CSST for the high-precision photometry, the weak-signal detection, and the related sciences. Here we present key design features, results of current ground tests, and suggested observing strategies of the MCI.

Qiqian Zhang, Zhou Fan, Gang Zhao, Ying Wu, Wei Wang, Kai Xiao, Hongrui Gu, Jie Zheng, Jingkun Zhao, Chun Li, Yuqin Chen, Haibo Yuan, Haining Li, Kefeng Tan, Yihan Song, Ali Luo, Nan Song, Yujuan Liu, Yaqian Wu
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Paper 62 — arXiv:2509.15112
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Paper 62 — arXiv:2509.15112

Reliable estimation of stellar surface gravity (log $g$) for a large sample is crucial for evaluating stellar evolution models and understanding galactic structure; However, it is not easy to accomplish due to the difficulty in gathering a large spectroscopic data set. Photometric sky survey using a specific filter, on the other hand, can play a substantial role in the assessment of log $g$. The Stellar Abundances and Galactic Evolution Survey (SAGES) utilizes eight filters to provide accurate stellar parameters for $\sim10^{7}$ stars, with its DDO51 intermediate-band filter specifically designed for robust log $g$ determination. In this work, the observed SAGES $u_{\rm SC}$ and $v_{\rm SAGES}$ photometry, the synthetic photometry in $g$, $r$, $i$, and DDO51 bands derived from \textit{Gaia} XP spectra are employed to investigate the importance of the DDO51 filter in the determination of log $g$. We applied machine-learning-based extinction correction and employed XGBoost models, trained on stellar parameters from LAMOST, to predict log $g$ using photometric data. By comparing model predicted log $g$ with LAMOST values, we find that including DDO51 filter improve the accuracies of log $g$ estimates by 21.0\% (from 0.224\,dex to 0.177\,dex) overall, and by 26.5\% (from 0.302\,dex to 0.222\,dex ) for GK-type stars, as compared to those obtained without DDO51. The DDO51 filter is also validated to be particularly effective for metal-poor stars ([Fe/H]$<$-1.0), where it significantly mitigates systematic biases. Our findings highlight the diagnostic power of the SAGES DDO51 filter, providing enhanced stellar characterization vital for future in-depth studies of the Milky Way.

Craig DeForest, Sarah Gibson, Ronnie Killough, Nick Waltham, Matt Beasley, Robin Colaninno, Glenn Laurent, Daniel Seaton, Marcus Hughes, Madhulika Guhathakurta, Nicholeen Viall, Raphael Attie, Dipankar Banerjee, Luke Barnar, Doug Biesecker, Mario Bisi, Volker Bothmer, Antonina Brody, Joan Burkepile, Iver Cairns, Jennifer Campbell, david Cheney, Traci Case, Amir Caspi, Rohit Chhiber, Matthew Clapp, Steven Cranmer, Jackie Davies, Curt de Koning, Mihir Desai, Heather Elliott, Samaiyah Farid, Bea Gallardo-Lacourt, Chris Gilly, Caden Gobat, Mary Hanson, Richard Harrison, Donald Hassler, Chase Henley, Alan Henry, Russell Howard, Bernard Jackson, Samuel Jones, Don Kolinski, Derek Lamb, Florine Lehtinen, Chris Lowder, Anna Malanushenko, William Matthaeus, David McComas, Jacob McGee, Huw Morgan, Divya Oberoi, Dusan Odstrcil, Chris Parmenter, Ritesh Patel, Francesco Pecora, Steve Persyn, Victor Pizzo, Simon Plunkett, Elena Provornikova, Nour Eddine Raouafi, Jillian Redfern, Alexis Rouillard, Kelly Smith, Keith Smith, Zachary Talpas, James Tappin, Arnaud Thernisien, Barbara Thompson, Samuel Van Kooten, Kevin Walsh, David Webb, William Wells, Matthew West, Zachary Wiens, Yan Yang
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Paper 65 — arXiv:2509.15131
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Paper 65 — arXiv:2509.15131

The Polarimeter to Unify the Corona and Heliosphere (PUNCH) mission is a NASA Small Explorer to determine the cross-scale processes that unify the solar corona and heliosphere. PUNCH has two science objectives: (1) understand how coronal structures become the ambient solar wind, and (2) understand the dynamic evolution of transient structures, such as coronal mass ejections, in the young solar wind. To address these objectives, PUNCH uses a constellation of four small spacecraft in Sun-synchronous low Earth orbit, to collect linearly polarized images of the K corona and young solar wind. The four spacecraft each carry one visible-light imager in a 1+3 configuration: a single Narrow Field Imager solar coronagraph captures images of the outer corona at all position angles, and at solar elongations from 1.5° (6 R$_\odot$) to 8° (32 R$_\odot$); and three separate Wide Field Imager heliospheric imagers together capture views of the entire inner solar system, at solar elongations from 3° (12 R$_\odot$) to 45° (180 R$_\odot$) from the Sun. PUNCH images include linear-polarization data, to enable inferring the three-dimensional structure of visible features without stereoscopy. The instruments are matched in wavelength passband, support overlapping instantaneous fields of view, and are operated synchronously, to act as a single ``virtual instrument'' with a 90° wide field of view, centered on the Sun. PUNCH launched in March of 2025 and began science operations in June of 2025. PUNCH has an open data policy with no proprietary period, and PUNCH Science Team Meetings are open to all.

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This paper introduces a segmented approach for solving constrained orbit transfer problems. The segments are connected through continuity constraints under the Theory of Functional Connections (TFC) mathematical framework that performs linear functional interpolation. This approach is further enhanced by a general vector formulation, from where the constrained functional is derived considering also a set of linear overdetermined constraints. Since we constrain vector instead of coordinates, this methodology allows to apply TFC to multiple and complex constraints composed by any types of nonlinear components included. We demonstrate the effectiveness of the method on Earth-to-Moon transfers, showing that this segmented approach achieves solutions with several orders of magnitude greater accuracy and efficiency in comparison with unsegmented orbit transfers.

In this study, we examined the nearby open clusters (OCs) Alessi 36 and Collinder 135. Their spatial proximity was assessed using photometric and astrometric data from \textit{Gaia} DR3. Likely member stars were identified based on a membership probability threshold ($P \geq 0.5$), yielding 230 members for Alessi 36 and 342 members for Collinder 135. The mean proper-motion components ($\mu_\alpha \cos\delta, \mu_\delta$) were determined as $(-9.681 \pm 0.072, 7.021 \pm 0.081)$ mas yr$^{-1}$ for Alessi 36 and $(-10.061 \pm 0.083, 6.256 \pm 0.095)$ mas yr$^{-1}$ for Collinder 135. The parallax-based distances ($d$) were found to be $278 \pm 7$ and $299 \pm 11$ pc, while their estimated ages ($t$) were $39 \pm 5$ and $36 \pm 5$ Myr for Alessi 36 and Collinder 135, respectively. The Galactic orbital analysis of Alessi 36 and Collinder 135 reveals nearly circular orbits with low eccentricities and minor fluctuations in their apogalactic and perigalactic distances. The maximum heights they attain above the Galactic plane are $0.035 \pm 0.001$ kpc for Alessi 36 and $0.074 \pm 0.003$ kpc for Collinder 135, supporting their classification as part of the young stellar disc population.

Amery Gration, David D. Hendriks, Payel Das, Daniel Heber, Robert G. Izzard

Ultrafaint dwarf (UFD) galaxies are dominated by dark matter, the distribution of which may be inferred from the kinematics of that galaxy's stellar population. Star-by-star observations are available for the satellite UFD galaxies of the Milky Way, making them uniquely good laboratories in which to test cosmological predictions at the smallest scales. However, the kinematics of these galaxies are complicated by the presence of binary stars, which alter the stellar velocity distribution. In particular these binary stars increase the galaxy's stellar velocity dispersion, which is related to the total galactic mass by the virial theorem. Without correctly eliminating or accounting for binary stars we may therefore overestimate the masses of UFD galaxies or even confuse globular clusters for UFD galaxies. Here we write down the probability density function for the observed line-of-sight (LOS) velocity of a stellar population containing both visual and spectroscopic binary stars, which we then use to determine the effect of those binary stars on the observed LOS velocity dispersion. For the coldest UFD galaxies the fractional increase in LOS velocity dispersion is of order one and for the coldest globular clusters is of order 100. However, if the stellar initial mass function is bottom light, as it may be for UFD galaxies and globular clusters, then both of these values increase by half a dex.

Collin T. Christy, Kate D. Alexander, Tanmoy Laskar, Noah Franz, Adelle J. Goodwin, Jeniveve Pearson, Edo Berger, Yvette Cendes, Ryan Chornock, Deanne Coppejans, Tarraneh Eftekhari, Raffaella Margutti, James C. A. Miller-Jones, Melanie Krips, Enrico Ramirez-Ruiz, David J. Sand, Richard Saxton, Manisha Shrestha, Sjoert van Velzen

We present a detailed radio study of the tidal disruption events (TDEs) AT 2020zso and AT 2021sdu. Both exhibit transient radio emission beginning shortly after optical discovery and persisting for several years. For AT 2020zso, we identify two distinct radio flares. The first arises soon after the optical peak, reaching a maximum $\sim1$ year post-discovery before fading. The second flare appears $\sim800$ days after discovery and results in the brief presence of two distinct components in the radio spectra, providing strong evidence for physically separate outflows. Both flares are consistent with non-relativistic outflows, with velocities $v\approx0.1-0.2c$ and energies $E\sim10^{49}$ erg, propagating through a Bondi-like circumnuclear medium. Our analysis supports a scenario in which the first outflow is accretion-driven, launched while the TDE disk is accreting at a relatively high Eddington fraction, whereas the second outflow is associated with a transition to an advection-dominated accretion flow. In contrast, the radio emission from AT 2021sdu is best explained by a slower ($v\approx0.03c$), less energetic outflow ($E\sim10^{48}$ erg), combined with diffuse, non-variable host emission that becomes dominant $\sim500$ days after discovery. Assuming free expansion, we infer an outflow launch date preceding the optical discovery date. This suggests that the outflow may originate from either the unbound stellar debris ejected during disruption or, alternatively, from a decelerating outflow. Our findings demonstrate the diversity of outflow properties in TDEs and highlight the observational challenges of interpreting late-time radio variability in the presence of host galaxy contamination.

Ian J. M. Crossfield, Eva-Maria Ahrer, Jonathan Brande, Laura Kreidberg, Joshua Lothringer, Caroline Piaulet-Ghorayeb, Jesse Polman, Luis Welbanks, James Kirk, Diana Powell, Niloofar Khorshid

this https URL . Resubmitted to ApJ (on 29 Aug) after referee review

JWST has revealed sulfur chemistry in giant exoplanet atmospheres, where molecules such as SO2 trace photochemistry, metallicity, and formation and migration. To ascertain the conditions that determine whether (or how much) SO2, H2S, and other sulfur-bearing species are present in exoplanet atmospheres, we present a grid of planetary atmospheres covering metallicities from 0.3-1000x Solar and temperatures from 250-2050 K. These models map out the 'SO2 shoreline,' the region of metallicity and irradiation for which SO2 may be sufficiently abundant to be detectable. SO2 is a sensitive indicator of metallicity; expected SO2 abundances also depend strongly on overall temperature and C/O ratio; the SO2 abundance depends surprisingly weakly on XUV irradiation, also weakly on Kzz (for Teq > 600 K), and is essentially independent of internal temperature. Despite its detection in a growing number of giant planets, SO2 is never the dominant sulfur-bearing molecule: depending on temperature and metallicity, H2S, S2, NS, SO, SH, and even S8 or atomic S are frequently as common (or more so) as SO2. Nonetheless SO2 remains the most easily detectable sulfur-bearing species, followed by H2S, though perhaps SO and SH could be detectable in some gas giants. Aside from a pressing need for additional observational constraints on sulfur, we also identify the need for future work to account for the effects of clouds and hazes, fully self-consistent atmospheric models, 2D and 3D models, a wider range of planetary masses and radii, and studies to measure and refine reaction rates and molecular opacities of sulfur-bearing species

Dimitri A. Gadotti (1), Camila de Sá-Freitas (2) ((1) Durham University, (2) ESO)

The presence of nuclear discs in barred disc galaxies has been demonstrated in studies on stellar structures and kinematics. It is thus imperative to establish their fundamental properties and scaling relations, which can help understanding their connection to other central stellar structures, including nuclear star clusters. In this Letter, we use results from the structural analysis and star formation histories of a sample of galaxies with nuclear discs to show the distributions of fundamental parameters and scaling relations. Our analysis shows that the nuclear disc mass-size relation, and the relation between the nuclear disc mass and the stellar mass of its host galaxy, are - at face value - different from the corresponding relations for nuclear star clusters, but marginally compatible given the uncertainties. This sets constraints to scenarios in which their formation is connected. We also find that the nuclear disc in the Milky Way is on the shorter end of the distribution of sizes set by nuclear discs in other galaxies. This is the first analysis of this kind for kinematically confirmed nuclear discs, and further understanding of the properties of the nuclear disc in the Milky Way and other galaxies is necessary to corroborate these results.

Jonathan Roberts (1, 2), William Thompson (3), Jason J. Wang (1, 2), Sarah Blunt (4, 1, 5), William O. Balmer (6, 7), Guillaume Bourdarot (8), Brendan P. Bowler (9), Gael Chauvin (10), Frank Eisenhauer (8), Thomas K. Henning (11), Jens Kammerer (12), Flavien Kiefer (13), Matthew A. Kenworthy (14), Pierre Kervella (13, 15), Sylvestre Lacour (13), A.-M. Lagrange (13, 16), Eric L. Nielsen (17), Laurent Pueyo (7), Emily Rickman (18), Olli Sipilä (8), Silvia Spezzano (8), Tomas Stolker (14), Alice Zurlo (19, 20) ((1) Center for Interdisciplinary Exploration and Research in Astrophysics (CIERA), Northwestern University, Evanston, USA, (2) Department of Physics and Astronomy, Northwestern University, Evanston, USA, (3) NRC Herzberg Astronomy and Astrophysics, Victoria, Canada, (4) Department of Astronomy and Astrophysics, University of California, Santa Cruz, USA, (5) NSF Astronomy and Astrophysics Postdoctoral Fellow, (6) Department of Physics and Astronomy, Johns Hopkins University, Baltimore, USA, (7) Space Telescope Science Institute, Baltimore, USA, (8) Max Planck Institute for Extraterrestrial Physics, Garching, Germany, (9) Department of Physics, University of California, Santa Barbara, USA, (10) Laboratoire Lagrange, Université Côte d'Azur, CNRS, Observatoire de la Côte d'Azur, Nice, France, (11) Max Planck Institute for Astronomy, Heidelberg, Germany, (12) European Southern Observatory, Garching, Germany, (13) LIRA, Observatoire de Paris, Université PSL, CNRS, Meudon, France, (14) Leiden Observatory, Leiden University, Leiden, The Netherlands, (15) French-Chilean Laboratory for Astronomy, CNRS and Universidad de Chile, Santiago, Chile, (16) Univ. Grenoble Alpes, CNRS, IPAG, Grenoble, France, (17) New Mexico State University, Las Cruces, USA, (18) European Space Agency (ESA), ESA Office, Baltimore, USA, (19) Instituto de Estudios Astrofísicos, Universidad Diego Portales, Santiago, Chile, (20) Millennium Nucleus on Young Exoplanets and their Moons (YEMS), Chile)

We present new VLTI/GRAVITY astrometry and updated orbit fits for the directly imaged companions YSES 1 b and HR 2562 B, substellar objects straddling the planet-brown dwarf boundary. Using high-precision astrometry, radial velocity (RV) data, and proper motions, we derive revised orbital parameters with orbitize! arXiv:1910.01756. For YSES 1 b, the inclusion of GRAVITY astrometry and a relative radial velocity measurement from arXiv:2409.16660 overcomes the traditional challenge of constraining eccentricities for distant companions, enabling the first orbit fit and yielding a constrained eccentricity of 0.44 (0.20). This represents the first full orbit fit for the system. Additionally, we calculate a median line-of-sight stellar obliquity of 12 (+11, -8) degrees, providing further insight into the system's dynamical architecture. For HR 2562 B, our analysis agrees with arXiv:2302.04893, confirming a low-eccentricity orbit (0.34 (0.20)) and an inclination of 87 (1) degrees. We find HR 2562 B's orbit to be nearly coplanar with the debris disk, with a mutual inclination of 3.7 (0.3) degrees. For both YSES 1 b and HR 2562 B the lower eccentricities favor an in situ formation scenario over extreme scattering or cloud fragmentation.

Wynne Turner, Andrei Cuceu, Paul Martini, J. Aguilar, S. Ahlen, A. Anand, D. Bianchi, D. Brooks, L. Casas, T. Claybaugh, A. de la Macorra, B. Dey, P. Doel, S. Ferraro, A. Font-Ribera, J. E. Forero-Romero, E. Gaztañaga, S. Gontcho A Gontcho, G. Gutierrez, H. K. Herrera-Alcantar, K. Honscheid, M. Ishak, R. Joyce, R. Kehoe, D. Kirkby, A. Kremin, O. Lahav, M. Landriau, L. Le Guillou, M. Manera, R. Miquel, A. Muñoz-Gutiérrez, S. Nadathur, G. Niz, N. Palanque-Delabrouille, W. J. Percival, C. Poppett, F. Prada, A. J. Ross, G. Rossi, E. Sanchez, D. Schlegel, M. Schubnell, H. Seo, J. Silber, D. Sprayberry, G. Tarlé, M. Walther, B. A. Weaver, R. Zhou, H. Zou

The standard cosmological analysis with the Ly$\alpha$ forest relies on a continuum fitting procedure that suppresses information on large scales and distorts the three-dimensional correlation function on all scales. In this work, we present the first cosmological forecasts without continuum fitting distortion in the Ly$\alpha$ forest, focusing on the recovery of large-scale information. Using idealized synthetic data, we compare the constraining power of the full shape of the Ly$\alpha$ forest auto-correlation and its cross-correlation with quasars using the baseline continuum fitting analysis versus the true continuum. We find that knowledge of the true continuum enables a $\sim10\%$ reduction in uncertainties on the Alcock-Paczyński (AP) parameter and the matter density, $\Omega_\mathrm{m}$. We also explore the impact of large-scale information by extending the analysis up to separations of $240\,h^{-1}\mathrm{Mpc}$ along and across the line of sight. The combination of these analysis choices can recover significant large-scale information, yielding up to a $\sim15\%$ improvement in AP constraints. This improvement is analogous to extending the Ly$\alpha$ forest survey area by $\sim40\%$.

Dust is essential to the evolution of galaxies and drives the formation of planetary systems. The challenge of inferring the origin of different presolar dust grains from meteoritic samples motivates forward modelling to understand the contributions of low- and high-mass stars to dust in our Solar System. In this work we follow the evolution of dust with tracer particles within a hydrodynamical simulation of a Milky Way-like isolated disc galaxy. We find that nearly half of the grains released from stars lose less than $10\%$ of their initial mass due to thermal sputtering in the interstellar medium (ISM), with an average degree of atomisation $\sim$$10\%$ higher for dust grains released by supernovae relative to asymptotic giant branch (AGB) star grains. We show through supernova remnant model variations that supernova (SN) dust survival is primarily shaped by the supernova bubble environment in the first million years (Myr) after the explosion rather than by its evolution during $10^2-10^3$ Myr in the ISM. The AGB/SN ratio of dust grains incorporated into newly formed stars approaches $0.8$ after a few hundred Myr of galactic evolution. Our analysis also shows that star-forming particles with short ($<$$10$ Myr) free-floating time-scales in the ISM are predominantly released from supernovae rather than AGB stars. This implies that the Solar System budget of short-lived radioactive isotopes such as $^{26}$Al, whose decay contributed to melting and differentiating planetesimals, should have been provided by massive stars with masses $M \gtrsim 8$ M$_{\odot}$.

We present pbhstat, a publicly available Python package designed to compute the mass function and total abundance of primordial black holes (PBHs) from a given primordial power spectrum. The package offers a modular framework using multiple statistical approaches, including Press-Schechter theory, peaks theory, and formalisms based on the non-linear compaction function. Currently, the implementation is limited to scenarios with nearly Gaussian initial conditions.

E. Koutsoumpou, J. A. Fernández-Ontiveros, K. M. Dasyra, L. Spinoglio

Cosmic rays (CRs), from active galactic nuclei (AGN) jets and supernovae (SNe), serve as a significant feedback mechanism influencing emission lines in narrow line region (NLR) clouds. These highly energetic particles, propelled by shocks, heat the interstellar medium (ISM) and modify its chemical composition. This study investigates the role of CRs, particularly in their ability to excite gas and align with observed line ratios across UV and optical diagnostics. We employ CLOUDY to explore CR ionization rate, ionization parameter, and initial hydrogen density effects on optical and mid-infrared (MIR) emission. Our analysis includes high-quality optical data from the Multi Unit Spectroscopic Explorer (MUSE) on the Very Large Telescope (VLT) for NGC 5728, supplemented by infrared observations from the James Webb Space Telescope (JWST). Our previous results indicate that CRs are instrumental in heating the inner regions of gas clouds, enhancing emission of low-ionization optical lines. Mid-infrared data reveal that emission lines like [Ar II] and [Ne II] within the JWST Mid-Infrared Instrument (MIRI) field of view are sensitive to CRs. In contrast, high-ionization lines (for example, [Ne V]) serve as robust tracers of photoionization insensitive to CRs. Moreover, mixed optical and MIR diagnostics offer insight into the relative roles of CRs and shocks, which often produce similar signatures in emission lines. We find that while both mechanisms can elevate certain line ratios, their influence on MIR diagnostics diverges: shocks and CRs affect low-ionization lines differently, allowing for a better understanding when multi-wavelength data are available. Our approach not only helps to resolve the degeneracy between metallicity and CR ionization but also enables the potential differentiation of shocks and CR-driven processes in AGN.

Lawrence Wiencke, James Brague, Ash Fox-Smith, Auston Froid, Levi Bar-On, Stephen Meyer, Josh Moses, Ben Stillwell (for the JEM-EUSO Collaboration)

The Probe of Extreme Multi-Messenger Astrophysics Balloon with Radio mission (PBR) will point above Earth's limb to measure PeV energy cosmic rays, and record star images to monitor optical focusing in situ. PBR will point below Earth's limb to search for earth-skimming neutrinos. PBR will also measure EeV energy cosmic rays by tilting as far down as the nadir direction. All of these searches will require changing and measuring the tilt angle of a single large integrated telescope and radio antenna assembly in the near space environment at 33 km above sea level over a mission duration as long as 50 days. In addition, the 1.1 m diameter entrance pupil of the telescope will be covered during the day by a shutter system to prevent sunlight from damaging the camera systems and opened at night to collect data. Here we present the design and status of the tilting system, the tilting monitors, the shutter system, the controller, and the preflight thermal vacuum testing process. The work draws on the experience of the 2023 Extreme Universe Space Observatory on a Super Pressure Balloon 2 mission.

Andrea Botteon, Turgay Caglar, Sibel Döner, Reinout J. van Weeren, Krista Lynne Smith

Interacting galaxy cluster pairs offer a unique opportunity to study the properties of the gas in the intracluster bridge connecting them. As a consequence of the encounter, both the X-ray and radio emission from the gas are expected to be enhanced by shocks and turbulence, facilitating their detection. PSZ2 G279.79+39.09 is likely an off-axis merging system at $z = 0.29$, with its two main components observed shortly after pericenter passage. In this paper, we investigate the presence of diffuse radio emission in this system. We observed the cluster pair with the MeerKAT UHF band (544-1088 MHz) for 7.5 h and uGMRT band 3 (300-500 MHz) for 8 h. These are the first targeted radio observations of this system. We discover diffuse synchrotron emission in the system, with indication of enhanced emission in the region bridging the cluster pair. The detection is based on MeerKAT UHF data, while uGMRT band 3 observations do not allow us to derive a stringent limit on the spectral index of the source. This emission is likely generated by the turbulence injected in the early stage after the cluster-cluster encounter. However, the study of its physical properties is limited by the current data. As other systems with multiple cluster components studied in recent years, this cluster pair represents an appealing target to probe nonthermal phenomena beyond the well-studied denser regions of the intracluster medium. While we report a new detection, our analysis highlights the need for multi-band observations to fully understand these sources.

Sean Bryan, Hugh Barnaby, Oketa Basha, C. Matt Bradford, Kathryn Chamberlin, Nicholas Cothard, Sumit Dahal, Thomas Essinger-Hileman, Alessandro Geist, Jason Glenn, Tracee Jamison-Hooks, Abarna Karthikeyan, Philip Mauskopf, Lynn Miles, Sanetra Bailey Newman, Cody Roberson, Karwan Rostem, Adrian Sinclair

We present the status and goals of the readout electronics system we are developing to support the detector arrays in the coronagraph instrument on the NASA Habitable Worlds Observatory (HWO) mission currently in development. HWO aims to revolutionize exoplanet exploration by performing direct imaging and spectroscopy of 25 or more habitable exoplanets, and to resolve a broad range of astrophysics science questions as well. Since exoplanet yield depends critically on the detector dark count rate, as we show in this paper, the ambitious goals of HWO require arrays of single-photon energy-resolving detectors. We argue that Kinetic Inductance Detectors (KIDs) are best suited to meet these requirements. To support the detectors required for HWO and future far-IR missions, at the required power consumption and detector count, we are developing a radiation-tolerant reconfigurable readout system for both imaging and energy-resolving single photon KID detector arrays. We leverage an existing RFSoC-based system we built for NASA balloons that has a power consumption of 30 Watts and reads out 2000-4000 detectors (i.e. 7-15 mW/pixel), and move to a radiation tolerant Kintex Ultrascale FPGA chip to bring low-power wide bandwidth readout to a space-qualified platform for the first time. This improves significantly over previous spaceflight systems, and delivers what is required for NASA's future needs: ~100,000 pixels with less than 1 kW total power consumption. Overall, the system we are developing is a significant step forward in capability, and retires many key risks for the Habitable Worlds Observatory mission.

Michael W. Healy-Kalesh, Manami Sasaki, Sean D. Points, Miroslav D. Filipović, Zachary J. Smeaton, Matthew J. Darnley, Knox S. Long, Sara Saeedi, Federico Zangrandi

A nova super-remnant (NSR) is a greatly-extended structure grown by repeated nova eruptions sweeping the surrounding material away from a nova into a dense outer shell and are predicted to form around all novae. To date, four NSRs are known, with three located in the Galaxy and one residing in M31. Here we present the discovery of the first NSR in the Large Magellanic Cloud and only the second extragalactic nova shell to be identified, hosted by the recurrent nova LMCN 1971-08a. The structure is coincident with the nova, has a circular morphology and is visible in narrowband H$\alpha$ and [S II] filters but very faint in [O III], as expected. HI data also potentially reveal the existence of a coincident structure. Further, with a diameter of ${\sim}200$ pc, this NSR is the largest example yet found, with models indicating an ${\sim}4130 \ \text{M}_{\odot}$ shell expanding at ${\sim}20 \ \text{km} \ \text{s}^{-1}$ into the surrounding medium and an age of $\sim$2.4 Myr. The existence of the NSR also suggests that LMCN 1971-08a may have a much shorter recurrence period than currently presumed.

The radio-frequency emissions produced by particle showers on Earth, resulting from cosmic rays (CRs) and ultra-high energy neutrinos (UHE-$\nu$) originating from astrophysical sources share significant similarities, enabling radio detectors initially designed for UHE-$\nu$ searches to also study CRs. The Askaryan Radio Array (ARA), an experiment currently operating within the ice at the South Pole, is primarily designed to detect UHE-$\nu$s. To date, ARA has deployed five stations, with each station equipped with antennas installed at depths up to 200 meters in the ice. Data recorded by ARA Station-2 (A2) suggest a potential CR origin for a subset of events identified in a UHE-$\nu$ search. This subset includes a double-pulse event potentially from a downward propagating CR-induced air shower, with in-air geomagnetic emission followed by in-ice Askaryan emission producing the two pulses. A detailed investigation of this CR candidate event using comprehensive simulations has been conducted with the goal of identifying the parameters of a CR-induced air shower that best match the experimentally observed quantities. We simulate predicted CR signals in ARA by combining an impacting CR shower simulation framework (FAERIE) with a realistic detector simulation (AraSim). We determine the event topology based on the vertex reconstruction of both the putative geomagnetic and Askaryan signals. After inferring the event geometry, we show that the simulation matches the observed time structure of the event (channel-by-channel relative signal arrival times) for the recorded event.

Meir E. Schochet, Penelope Planet, Zachary R. Claytor, Jamie Tayar, Adina D. Feinstein

Stars exhibit a range of variability periods that depend on their mass, age, and evolutionary stage. For space-based photometric data, convolutional neural networks (CNNs) have demonstrated success in recovering and measuring periodic variability from photometric missions like Kepler and TESS. All-sky ground-based surveys can have similar if not longer baselines than space-based missions, however these datasets are more challenging to work with due to irregular sampling, more complex systematics, and larger data gaps. In this work, we demonstrate that CNNs can be used to derive variability periods from ground-based surveys. From the All-Sky Automated Survey for Supernovae (ASAS-SN) we recover 208,260 variability periods between 1-30 days, approximately 60% of which are new detections. We recover periods for active RSCVn, anomalous sub-subgiants, and cool dwarfs that are consistent with previously measured rotation periods, while periods for stars above the Kraft break are generally spurious. We also identify periodic signals in tens of thousands of giants stars which correspond to frequencies of stellar oscillations rather than rotation. Our results highlight that CNNs can be used on sparsely sampled ground-based photometry and may prove useful for upcoming observations from the Vera C. Rubin Observatory's Legacy Survey of Space and Time (LSST).

R. Fuentetaja, C. Cabezas, Y. Endo, M. Agúndez, A. Godard Palluet, F. Lique, B. Tercero, N. Marcelino, P. de Vicente, J. Cernicharo

We performed a detailed analysis of the isotopologues with 13C, 34S, 33S, and 36S of the sulphur-bearing molecules CS, CCS, CCCS,HCS+, HCCS+, and H2CS towards TMC-1 using the QUIJOTE1. The observations were obtained with the Yebes radio telescope. Observations with the IRAM 30m of the most abundant isotopologues of these species are also presented and used to estimate volume densities and to constrain the excitation conditions. We report the first detection in space of C13C34S, CC33S, CCC33S, HC33S+, and HCC34S+. C36S is also detected for the first time in a cold object. We also complemented with maps that provide the spatial distribution of most of these species. Using the available collisional rate coefficients for each species, we modeled the observed line intensities using the large velocity gradient method for the radiative transfer. We report the most complete analysis of the column densities of the CnS family and to compare the abundance ratios of all detected isotopologues. Adopting a T_k for TMC-1 of 9K, we found that n(H2)=0.9-1.5X10^4cm-3 can explain the observed decline in intensity with increasing J. We derived the rot. constants for the C13C34S, CC33S, CCC33S, HC33S+, and HCC34S+ isotopologues from new laboratory data and complemented them with the frequencies of the observed lines. We find that all S isotopologues are consistent with solar isotopic abundance ratios. Accurate 12C/13C abundances were derived and, as previously suggested, the 13C isotopologues of CCS and CCCS show strong abundance anomalies depending on the position of the substituted carbon. Nevertheless, the 12C/13C abundance ratio is practically identical to the solar value for CS, HCS+, and H2CS. We also searched for the isotopologues of other S-bearing molecules. The expected intensities for their 34S and 13C isotopologues are too low to be detected with the present sensitivity of the QUIJOTE, however.

Shifra Mandel (1), Kaya Mori (1), Anna Ciurlo (2), Paul A. Draghis (3), Noa Grollimund (4), Gaurava K. Jaisawal (5), Chichuan Jin (6), Benjamin Levin (1), Lorenzo Marra (7), Eric Miao (1), Maxime Parra (8), Mark Reynolds (9), Sean A. Granados (2), Matteo Bachetti (10), Fiamma Capitanio (7), Nathalie Degenaar (11), Charles J. Hailey (1), JaeSub Hong (12), Sara Motta (13), Gabriele Ponti (13), Michael M. Shara (14), Megumi Shidatsu (8), John A. Tomsick (15), Randall Campbell (16), Stéphane Corbel (4), Rob Fender (17), Andrea Ghez (2), Jonathan Grindlay (12), Matthew W. Hosek Jr. (2), Kai Matsunaga (18), Romana Mikušincová (7), Melania Nynka (3), Grace Sanger-Johnson (19), Giovanni Stel (13), Antonella Tarana (7), Rudy Wijnands (11), Shuo Zhang (19) ((1) Columbia Astrophysics Laboratory, (2) UCLA Department of Physics and Astronomy, (3) MIT Kavli Institute for Astrophysics and Space Research, (4) Université Paris Cité, Université Paris-Saclay, (5) DTU Space, Technical University of Denmark, (6) National Astronomical Observatories, Chinese Academy of Sciences, (7) INAF Istituto di Astrofisica e Planetologia Spaziali, (8) Department of Physics, Ehime University, (9) Department of Astronomy, Ohio State University, (10) INAF-Osservatorio Astronomico di Cagliari, (11) Anton Pannekoek Institute for Astronomy, University of Amsterdam, (12) Center for Astrophysics | Harvard \&amp; Smithsonian, (13) INAF-Osservatorio Astronomico di Brera, (14) Department of Astrophysics, American Museum of Natural History, (15) Space Sciences Laboratory, University of California, Berkeley, (16) W.M. Keck Observatory, (17) Astrophysics, Department of Physics, University of Oxford, (18) Department of Physics, Graduate School of Science, Kyoto University, (19) Department of Physics and Astronomy, Michigan State University)

For the first time in nearly a decade, a new, bright transient was detected in the central parsec (pc) of the Galaxy. MAXI J1744-294 was never observed in outburst prior to January 2025. We present the results of a broadband, multi-wavelength study of this enigmatic source, including data from the NuSTAR, Chandra, XMM-Newton, Swift, and NICER X-ray telescopes, as well as complementary radio and near-infrared observations. We find that MAXI J1744-294 remained in the bright/soft state throughout the first months of 2025. Spectral hardening was observed in April 2025, followed by a decline in flux. Based on the spectral and temporal characteristics of the source, we identify MAXI J1744-294 as a candidate black hole (BH) low-mass X-ray binary (LMXB) $-$ the fourth candidate BH transient discovered within a (projected) distance of one pc from the Galactic supermassive black hole Sgr A*. This discovery provides further evidence for a cusp of BH-LMXBs in the central pc of our Galaxy, as argued for in previous observational work and suggested by analytical and theoretical work. Our multi wavelength study, involving a complementary range of observatories and spanning different outburst states, can serve as a model for future time domain astrophysics research.

William E. Harris, Marta Reina-Campos, Kaitlyn E. Keatley, Marusa Bradac, Nicholas S. Martis, Adam Muzzin, Gael Noirot, Ghassan T. E. Sarrouh, Marcin Sawicki, Chris J. Willott, Samantha C. Berek

Deep JWST imaging of the massive galaxy cluster MACS0417.5-1154, at redshift z=0.443, reveals a huge population of globular clusters (GCs) and Ultra-Compact Dwarfs (UCDs) primarily distributed around its single central giant galaxy (BCG). We present NIRCam/SWC photometry of the GC system in four bands (F090W, F115W, F150W, F200W). The spatial distribution of the system matches well in radial and ellipticity profile with the high elongation (b/a = 0.5) of the BCG halo light. The total GC population within MACS0417 is estimated to be near 1.5 x 10^5, similar to the systems in Abell 2744, Coma, and other galaxy clusters with comparable masses. With similar results for GC photometry in hand from other lensing clusters at a range of redshifts, it is now possible to trace on purely observational grounds the luminosity evolution of GC systems over many Gigayears of lookback time, as seen through their color-magnitude diagrams. We show this sequence for five systems reaching to lookback times of more than 7 Gyr. A systematic change in the GC/UCD sequence with lookback time is clearly visible, near what is expected for age-fading of a simple stellar population with time. Lastly, we evaluate the effectiveness of the various JWST NIRCam filters for broadband photometry of GC systems as a function of redshift, as an aid to planning further studies.

We performed \textit{N}-body/SPH simulations of isolated spiral galaxies with various bulge-to-disk mass ratios ($M_{\rm bulge}/M_{\rm disk}$) from 0.02 to 0.2 to investigate mass transport from galactic scales (10 kpc) down to circumnuclear disk scales ($\lesssim$ 100 pc). Our analysis revealed these main findings, (1) Gravitational torque from stellar spiral arms causes gas accretion with $\sim1$ $M_\odot$ ${\rm yr}^{-1}$ along the gas spiral arms from a few kpc to a few 100 pc scale. The density of accreting gas is a few 100 ${\rm cm^{-3}}$, comparable to the gas arms. The pressure gradient force is over an order of magnitude weaker than the stellar gravitational torque. (2) Gravitational torque from barred structure causes episodic gas clump accretion with $\sim1$ $M_\odot$ ${\rm yr}^{-1}$ on timescales of 10 Myr from kpc to a few 100 pc scale. The densities of these clumps exceed 700 ${\rm cm^{-3}}$, and this accretion occurs along elliptical orbits with a delayed phase relative to the bar potential \citep{wada1994}. (3) Episodic gas clumpy accretion is important for galactic center instability, confirmed by $M_{\rm bulge}/M_{\rm disk}$ = 0.02 but not by $M_{\rm bulge}/M_{\rm disk}$ = 0.1 and 0.2. This difference occurs because in the bulge-dominated potentials, bar instability is suppressed, and rapid gas clumps accretion does not occur. These findings suggest that gas clump accretion events driven by bars could be a source of high-density gas to the galactic center of the spiral galaxy, potentially promoting temporary activity in the galactic center.

Kaito Ninoyu, Keisuke Uchiyama, Shinya Yamada, Ryota Hayakawa, Shunji Kitamoto, Nao Kominato, Takayoshi Kohmura, Misaki Mizumoto, Yuusuke Uchida, Toru Tamagawa, Ryota Tomaru, Seoru Ito

We report the first statistically significant detection of X-ray polarization from the high-mass X-ray binary (HMXB) 4U 1700-377, observed using the Imaging X-ray Polarimetry Explorer (IXPE). A polarization degree exceeding 10% was detected above 5 keV, placing it among the highest polarization observed in HMXBs to date. The observation was conducted over a full orbital period of the binary system, during which several sporadic and instantaneous flares were detected. We identify a clear correlation between the polarization degree and orbital phase, with the highest polarization occurring just before and after the eclipse, reaching over 20% for a few tens of ks. These results suggest that the scattering medium responsible for the observed polarization is spatially localized between the compact object and the O-type companion star, likely created by large-scale inhomogeneities in the stellar wind and its interaction with the compact star's emission. We also explore the roles of disk winds and orbital reflection in the observed polarization variability. While both mechanisms contribute to the polarization, the substantial increase in polarization before and after the eclipse cannot be fully explained by these models alone, suggesting that the involvement of additional factors. The properties of the X-ray polarization observed by IXPE provide new insights into the accretion processes, X-ray emission, and wind structure in 4U 1700-377, advancing our understanding of their complex environments and the nature of the compact objects within.

SPHEREx, a recently launched astronomy mission, detected a bright 1.083 micron emission feature in the commissioning data. The PI group attributed this feature to the He I 1.0833 micron triplet line. Here, I review the physics and aeronomy of this well-known line of atmospheric origin. SPHEREx is in a dawn-dusk sun-synchronous polar orbit, circling the earth nearly 15 times a day and observing close to the terminator plane. With a height of 650 km, SPHEREx is located in the upper thermosphere that is dominated by atomic oxygen and helium. The He I line is a result of resonance scattering of solar photons by metastable helium atoms. It appears that SPHEREx has the capacity to provide a rich dataset (global, daily, and 2-minute cadence) of column density of metastable helium in the upper thermosphere. As an example of this assertion, with data from just one orbit, the winter helium bulge was readily seen. Rapid variations in the column density of metastable helium is seen over the south pole which is probably due to spatial structure in the distribution of metastable helium as well as solar activity. Helium in the thermosphere is of considerable interest to operators of low-earth orbiting (LEO) satellites, since drag in the thermosphere is the primary cause of the decay of these satellites. SPHEREx, along with on-going ground-based studies (passive NIR spectroscopy, lidar, incoherent scatter radar), is poised to contribute to this topic.

J.Kataoka, S.Ogasawara, R.Mori, K.Yamamoto, A.R.Joshi, S.Kojima, K.Sato, K.S.Tanaka, K.Watanabe, M.Yasuda, H.Kobayashi, D.Kobayashi, A.Ohira, Y.Amaki, Y.Arai, K.Tashirio, K.Otsubo, Y.Ozeki, Y.Kawaguchi, D.Yoshimura, H.Yoshida, K.Takahashi, S.Masaki, N.Yamada, K.Oikawa, E.Zamami, K.Miyamoto, T.Chujo, H.Nakanishi, T.Tomura, S.Hayatsu, M.Fukuda, H.Seki, S.Joshima, Y.Yatsu

The Compton camera is a gamma-ray imaging device developed in the 1970s. In the 1990s, the COMPTEL detector onboard the CGRO was the first to utilize a Compton camera for MeV all-sky survey observations. Recently, various Compton cameras have been developed using scintillators, semiconductors, and gas detectors, some of which are intended for future small satellite missions as well as medical applications. However, the image obtained by a Compton camera has strong artifacts owing to the overlap of the Compton cones or the arcs, which degrade the resolution and sensitivity of the image. In this study, we revisit the adaptive ARM cut that significantly reduces artifacts when the direction of gamma ray emitting source is already known. This approach complements the statistically well-defined method based on the response function in the three-dimensional data space of scattering direction (\chi, \psi) and scattering angle \theta, but it is more direct, intuitive, and simplifies the extraction of spectra in astronomical observations of point-like sources. Using a Compton camera, INSPIRE, onboard the ultra-small satellite GRAPHIUM as an example, we numerically evaluated the extent of background reduction to estimate simulation-based sensitivity. The method was also applied to actual measurements using a quarter-scale prototype of INSPIRE to extract spectra from multiple sources within the same field of view.

François L. H. Tissot, Christoph Burkhardt, Aleksandra Kuznetsova, Andreas Pack, Martin Schiller, Fridolin Spitzer, Elishevah M. M. E. Van Kooten, Teng Ee Yap

How do planetary systems, in general, and our own Solar System (SS), in particular, form? In conjunction, Astronomy and Isotope Cosmochemistry provide us with powerful tools to answer this age-old question. In this contribution, we review recent advances in our understanding of circumstellar disk evolution, including infall and disk processes, as explored through astrophysical models and nucleosynthetic isotope anomalies of SS materials. Astronomically, filamentary structures and anisotropy are observed across the dynamic range of star formation and disk substructures are found to be ubiquitous, highlighting how star- and planet-forming environments are far more complex and dynamic than previously thought. Isotopically, two decades of investigation of nucleosynthetic anomalies in bulk meteorites and refractory inclusions have produced a rich dataset, revealing the existence of pervasive heterogeneity in the early SS, both at the large- (i.e., NC-CC dichotomy) and fine-scale (i.e., trends within the NC group). Using an updated data compilation, we review the systematics and emerging structures of these anomalies as a function of their nucleosynthetic origin. We present the two main families of models - inheritance vs. unmixing - that have been proposed to explain the origin of the observed isotope heterogeneities, and discuss their respective implications for cloud infall and thermal processing in the disk. We also discuss how the extension of nucleosynthetic anomaly analyses to other chondritic components (Ameboid Olivine Aggregates, chondrules, matrix) has started to yield insights into transport, processing and mixing of dust in the disk. Limitations, open questions and key avenues for future work are presented in closing.

Marc Audard, Hisamitsu Awaki, Ralf Ballhausen, Aya Bamba, Ehud Behar, Rozenn Boissay-Malaquin, Laura Brenneman, Gregory V. Brown, Lia Corrales, Elisa Costantini, Renata Cumbee, Maria Diaz Trigo, Chris Done (Durham-CEA, UK), Tadayasu Dotani, Ken Ebisawa, Megan Eckart, Dominique Eckert, Teruaki Enoto, Satoshi Eguchi, Yuichiro Ezoe, Adam Foster, Ryuichi Fujimoto, Yutaka Fujita, Yasushi Fukazawa, Kotaro Fukushima, Akihiro Furuzawa, Luigi Gallo, Javier A. Garcia, Liyi Gu, Matteo Guainazzi, Kouichi Hagino, Kenji Hamaguchi, Isamu Hatsukade, Katsuhiro Hayashi, Takayuki Hayashi, Natalie Hell, Edmund Hodges-Kluck, Ann Hornschemeier, Yuto Ichinohe, Manabu Ishida, Kumi Ishikawa, Yoshitaka Ishisaki, Jelle Kaastra, Timothy Kallman, Erin Kara, Satoru Katsuda, Yoshiaki Kanemaru, Richard Kelley, Caroline Kilbourne, Shunji Kitamoto, Shogo Kobayashi, Takayoshi Kohmura, Aya Kubota, Maurice Leutenegger, Michael Loewenstein, Yoshitomo Maeda, Maxim Markevitch, Hironori Matsumoto, Kyoko Matsushita, Dan McCammon, Brian McNamara, Francois Mernier, Eric D. Miller, Jon M. Miller, Ikuyuki Mitsuishi, Misaki Mizumoto (Fukuoka, Japan), Tsunefumi Mizuno, Koji Mori, Koji Mukai, Hiroshi Murakami, Richard Mushotzky, Hiroshi Nakajima, Kazuhiro Nakazawa, Jan-Uwe Ness, Kumiko Nobukawa, Masayoshi Nobukawa, Hirofumi Noda, Hirokazu Odaka, Shoji Ogawa, Anna Ogorzalek, Takashi Okajima, Naomi Ota, Stephane Paltani, Robert Petre, Paul Plucinsky, Frederick Scott Porter, Katja Pottschmidt, Kosuke Sato, Toshiki Sato, Makoto Sawada, Hiromi Seta, Megumi Shidatsu, Aurora Simionescu, Randall Smith, Hiromasa Suzuki, Andrew Szymkowiak, Hiromitsu Takahashi, Mai Takeo, Toru Tamagawa

this https URL (Nature September 17 2025)

Accretion discs in strong gravity ubiquitously produce winds, seen as blueshifted absorption lines in the X-ray band of both stellar mass X-ray binaries (black holes and neutron stars), and supermassive black holes. Some of the most powerful winds (termed Eddington winds) are expected to arise from systems where radiation pressure is sufficient to unbind material from the inner disc ($L\gtrsim L_{\rm Edd}$). These winds should be extremely fast and carry a large amount of kinetic power, which, when associated with supermassive black holes, would make them a prime contender for the feedback mechanism linking the growth of those black holes with their host galaxies. Here we show the XRISM Resolve spectrum of the Galactic neutron star X-ray binary, GX 13+1, which reveals one of the densest winds ever seen in absorption lines. This Compton-thick wind significantly attenuates the flux, making it appear faint, although it is intrinsically more luminous than usual ($L\gtrsim L_{\rm Edd}$). However, the wind is extremely slow, more consistent with the predictions of thermal-radiative winds launched by X-ray irradiation of the outer disc, than with the expected Eddington wind driven by radiation pressure from the inner disc. This puts new constraints on the origin of winds from bright accretion flows in binaries, but also highlights the very different origin required for the ultrafast ($v\sim 0.3c$) winds seen in recent Resolve observations of a supermassive black hole at similarly high Eddington ratio.

Charmi Bhatt (1 and 2), Jan Cami (1, 2 and 3), Els Peeters (1, 2 and 3), Nicholas Clark (1), Paula Moraga Baez (4), Kevin Volk (5), G. C. Sloan (5 and 6), Joel H. Kastner (4 and 7 and 8), Harriet L. Dinerstein (9), Mikako Matsuura (10), Bruce Balick (11), Kathleen E. Kraemer (12), Kay Justtanont (13), Olivia Jones (14), Raghvendra Sahai (15), Isabel Aleman (16), Michael J. Barlow (17), Jeronimo Bernard-Salas (18 and 19), Joris Blommaert (20), Naomi Hirano (21), Patrick Kavanagh (22), Francisca Kemper (23, 24 and 25), Eric Lagadec (26), J. Martin Laming (27), Frank Molster (28), Hektor Monteiro (29 and 30), Anita M. S. Richards (31), N. C. Sterling (32), Maryam Torki (23), Peter A. M. van Hoof (33), Jeremy R. Walsh (34), L. B. F. M. Waters (35 and 36), Roger Wesson (29 and 17), Finnbar Wilson (29), Nicholas J. Wright (37), Albert A. Zijlstra (31 and 38) ((1) Department of Physics and Astronomy, University of Western Ontario, (2) Institute for Earth and Space Exploration, University of Western Ontario, (3) SETI Institute, (4) Center for Imaging Science, Rochester Institute of Technology, (5) Space Telescope Science Institute, (6) Department of Physics and Astronomy, University of North Carolina, (7) School of Physics and Astronomy, Rochester Institute of Technology, (8) Laboratory for Multiwavelength Astrophysics, Rochester Institute of Technology, (9) Department of Astronomy, University of Texas at Austin, (10) Cardiff Hub for Astrophysics Research and Technology (CHART), School of Physics and Astronomy, Cardiff University, (11) Department of Astronomy, University of Washington, (12) Institute for Scientific Research, Boston College, (13) Chalmers University of Technology, Onsala Space Observatory, (14) UK Astronomy Technology Centre, Royal Observatory, (15) Jet Propulsion Laboratory, California Institute of Technology, (16) Laboratorio Nacional de Astrofisica, (17) Department of Physics and Astronomy, University College London, (18) ACRI-ST, Centre d'Etudes et de Recherche de Grasse (CERGA), (19) INCLASS Common Laboratory, (20) Astronomy and Astrophysics Research Group, Department of Physics and Astrophysics, Vrije Universiteit Brussel, (21) Academia Sinica Institute of Astronomy and Astrophysics, (22) Department of Physics, Maynooth University, (23) Institut de Ciencies de l'Espai (ICE, CSIC), (24) ICREA, (25) Institut d'Estudis Espacials de Catalunya (IEEC), (26) Universite Cote d'Azur, Observatoire de la Cote d'Azur, CNRS, Lagrange, (27) Space Science Division, Naval Research Laboratory, (28) Leidse instrumentmakers School, (29) Cardiff Hub for Astrophysics Research and Technology (CHART), School of Physics and Astronomy, Cardiff University, (30) Instituto de Fisica e Quimica, Universidade Federal de Itajuba, (31) Jodrell Bank Centre for Astrophysics, Department of Physics &amp; Astronomy, The University of Manchester, (32) University of West Georgia, (33) Royal Observatory of Belgium, (34) European Southern Observatory, (35) Department of Astrophysics/IMAPP, Radboud University, (36) SRON Netherlands Institute for Space Research, (37) Astrophysics Research Centre, Keele University, (38) School of Mathematical and Physical Sciences, Macquarie University)

Planetary nebulae are sites where ejected stellar material evolves into complex molecules, but the precise physical conditions and chemical routes that govern these processes are unclear. The presence of abundant carbon-rich molecules in O-rich environments poses particular challenges. Here we report the first detection of methyl cation (CH3+) in any planetary nebula, observed in the O-rich nebula NGC 6302 using JWST MIRI/MRS observations. CH3+ is a key driver of organic chemistry in UV-irradiated environments. Spatially resolved observations reveal that CH3+ is co-located with 12CO, H2, H II, HCO+, and Polycyclic aromatic hydrocarbons (PAHs). LTE modelling of the CH3+ emission yields excitation temperatures of 500-800K in the inner bubble and torus, rising to 1000-2000K in the outer bubble of NGC 6302, with column densities ranging from ~10^11 to 10^13 cm^-2. This detection demonstrates that hydrocarbon radical chemistry must be incorporated into planetary nebulae chemical models. Further near-IR observations are crucial to map different chemical networks operating in these environments.

This paper extends our previous study of gyro-emission by energetic electrons in the magnetospheres of rapidly rotating, magnetic massive stars, through a quantitative analysis of the role of Coulomb collisions with thermal electrons from stellar wind material trapped within the centrifugal magnetosphere (CM). For a dipolar field with aligned magnetic and rotational axes, we show that both gyro-cooling along magnetic loops and Coulomb cooling in the CM layer have nearly the same dependence on the magnitude and radial variation of magnetic field, implying that their ratio is a global parameter that is largely independent of the field. Analytic analysis shows that, for electrons introduced near the CM layer around a magnetic loop apex, collisional cooling is more important for electrons with high pitch angle, while more field-aligned electrons cool by gyro-emission near their mirror point close to the loop base. Numerical models that assume a gyrotropic initial deposition with a gaussian distribution in both radius and loop co-latitude show the residual gyro-emission is generally strongest near the loop base, with highly relativistic electrons suffering much lower collisional losses than lower-energy electrons that are only mildly relativistic. Finally, we briefly discuss the potential applicability of this formalism to magnetic ultracool dwarfs, for which VLBI observations indicate incoherent radio emission to be concentrated around the magnetic equator, in contrast to our predictions here for magnetic hot stars. We suggest that this difference could be attributed to either a lower ambient density of thermal electrons, or more highly relativistic non-thermal electrons, both of which would reduce the relative importance of the collisional cooling explored here.

The blazar TXS 0506+056 has been suggested to be a potential high-energy neutrino source thanks to the observations of IceCube, which found outburst-like neutrino emissions during 2014-2015 and 2017 in the transient emission search, and a $3.5\sigma$ local significance in a 10-year time-integrated search. The conventional one-zone jet model cannot explain the observed neutrino flux during outbursts due to the constraint from the X-ray flux, leading to proposals of multi-zone models (e.g. two-zone model) with multiple radiation zones. In literature, it has been shown that multi-zone models may consistently explain the high-state neutrino emission and the multi-wavelength emission of TXS 0506+056, while the quasi-steady-state long-term emission has not been well studied. In this work, we investigate a physically based model for the quasi-steady-state neutrino and electromagnetic radiation under the same framework, and successfully reproduce the multi-messenger emission of TXS 0506+056.

M. Kıyami Erdim, Emine Gülmez, Murat Hüdaverdi

In this study, we investigate the chemical enrichment and structural evolution of the isolated elliptical relic galaxy Mrk1216 through X-ray observations. As a red-nugget relic, Mrk1216 provides a rare window into the early Universe, owing to its minimal interaction with the surrounding environment. Using data from the XMM-Newton telescope, we model the X-ray emission of its interstellar medium to derive radial temperature and abundance profiles. We find that the central region exhibits an elevated [Mg/Fe] ratio compared to typical early-type galaxies, consistent with a brief but intense star formation episode during its early assembly-a hallmark of relic systems. The nearly flat SNIa ratio profile ($R_{Ia} \sim 0.17$) extending to $\sim0.42R_{500}$ supports an early-enrichment scenario. These results highlight the importance of relic galaxies as benchmarks for studying early galaxy evolution and chemical enrichment. Future high-resolution missions and more advanced theoretical models incorporating more realistic initial mass functions are needed to fully assess their implications.

Relatively blue light extends beyond a spiral disk from a radius of ~5 kpc out to ~14 kpc from the center of NGC 1275. Analyses of its spectrum and broadband colors reveal a population of young stars having sub-solar metallicities superposed on a dominant population of old stars having super-solar metallicities. The young stars have a characteristic age of ~160 Myr and may span ages of a few hundred Myr, similar to that of stars comprising the central spiral disk, and a total mass about one-third that of this disk for a combined stellar mass (at birth) of ~4 $\times$ 10$^9$ $\rm M_\odot$. A multitude of arc-like features embedded in the extended blue light have brightnesses comparable to the somewhat older (~500 Myr) super star clusters (SSCs) projected against the central spiral disk. The SSCs have a relatively shallow mass function, suggesting that the tidal disruption of an initially larger population that we estimate could have had an initial total mass (far) exceeding ~1 $\times$ 10$^9$ $\rm M_\odot$ gave rise to the extended blue light -- the arc-like features corresponding to stellar streams tracing disrupted star clusters -- and perhaps also the central spiral disk. We speculate that, beginning about 500 Myr ago, an enhanced episode of AGN activity in NGC 1275, leaving still visible X-ray bubbles, induced vigorous cooling of the intracluster medium to fuel the formation of numerous star clusters: many were tidally disrupted to leave bluish light at the inner region of this galaxy, with the survivors being the SSCs projected against the central spiral disk.

Interstellar dust plays a central role in the evolution of galaxies by shaping star formation, altering observed stellar properties, and redistributing radiation across the electromagnetic spectrum. In the Milky Way, dust is concentrated in the Galactic disk and often associated with large-scale structures such as spiral arms and molecular clouds. Here we present a detailed analysis of the vertical distribution and substructure of interstellar dust using a sample of approximately 23 million stars from literature with high-precision extinction measurements. We derive three-dimensional dust density profiles along various sightlines and fit vertical dust distributions using both single and double exponential disk models across 12 Galactocentric radial bins from $\sim$6 to $\sim$12\,kpc. We show that a two-component disk model--comprising a ``thin'' and a ``thick'' dust disk--provides a better fit to the vertical dust profile than a single exponential disk, as indicated by Bayesian Information Criterion (BIC) comparisons. The thin and thick disks have average scale heights of $81.0 \pm 6.7$\,pc and $152.0 \pm 7.0$\,pc, respectively. Our results also identify significant dust substructures, which align well with known spiral arms, molecular clouds, and star-forming regions.

As a characteristic feature of the spectrum, the emission line carries critical information on the underlying physics of the radiation. After extensive efforts in decades, the first high-significant detection of a series of emission lines evolving from 37 MeV to 6 MeV has been detected in the ever-bright gamma-ray burst GRB 221009A. However, the physical mechanism of the entire evolutionary trend of the lines remains elusive. To provide a self-consistent interpretation, we propose a novel scenario in which the photons of the line undergo a radiation transfer process called down-Comptonization after generation by the electron--positron pair annihilation. By incorporating the gamma-ray burst dynamical evolution, we systematically reproduce the observed evolution of the central energy, width, and flux of the emission line and further impose stringent constraints on the production of high-energy emission lines in general. Our study provides a new direction to the research of extreme cosmic bursts.

Isocurvature perturbations expected from multi-field inflation models can leave unique signatures in the early Universe, but remain weakly constrained, especially on small scales. In this work, we investigate the constraining power of one-point statistics (variance and skewness) of the 21cm brightness temperature during Cosmic Dawn and the Epoch of Reionization, using semi-numerical simulations from 21cmFAST. We model both adiabatic and cold dark matter isocurvature modes, exploring their impact on the matter power spectrum, the timing of structure formation, and the evolution of neutral hydrogen. By varying astrophysical parameters as well as isocurvature fraction and spectral index, we quantify their respective effects on the 21cm power spectrum and on one-point statistics. Our results show that while variance is highly sensitive to the timing of cosmic events and provides tight constraints on isocurvature parameters, skewness is more strongly affected by astrophysical uncertainties and observational noise. Incorporating realistic instrumental noise based on SKA configurations, we perform a Fisher analysis and demonstrate that 21cm variance measurements can constrain the isocurvature fraction down to the sub-percent level, though a strong degeneracy with the spectral index remains. We discuss the importance of complementary probes, such as the 21cm forest and galaxy surveys, to break these parameter degeneracies. Our findings highlight the power of 21cm one-point statistics as robust and independent tools for probing early-Universe physics beyond what is accessible with traditional power spectrum analyses.

We investigate the effects of Lorentz invariance violation (LIV) on photon interactions, considering both intergalactic propagation (Breit-Wheeler process) and atmospheric interactions (Bethe-Heitler process). By incorporating LIV into the theoretical framework, we analyze how it modifies key quantities such as the cross section, threshold energy, and mean free path of photons traveling through intergalactic space. In addition, we study its impact on extensive air showers initiated by high-energy photons, demonstrating that LIV can alter the cross section of the primary interaction in the atmosphere. Additionally, we also test the photon interactions in the Earth crust, to evaluate if they can induce upward-going showers. Our results highlight the necessity of accounting for both propagation effects in intergalactic space and interactions in the atmosphere when evaluating LIV signatures. Even small deviations from Lorentz invariance can lead to measurable changes in astroparticle propagation and photon dynamics, offering new opportunities to test quantum gravity theories through high-energy astrophysical observations.

Diffuse emission in gamma-rays and neutrinos are produced by the interaction of cosmic rays with the interstellar medium. Below some hundreds of TeV, the sources of these cosmic rays are most likely Galactic. Hence, observations of high-energy gamma-rays and neutrinos can be used to probe the flux of cosmic rays in other parts of the Galaxy. Supernova remnants are usually considered as the prime candidate for the acceleration of Galactic cosmic rays. They inject cosmic rays in a point-like and specific time-dependent manner. As the precise positions and ages of the sources are not known, predictions must be obtained in a stochastic model. At GeV energies, the distribution of sources can be approximated with a smoothly varying spatial and temporal source density. At hundreds of TeV, however, the point-like nature matters as less sources contribute effectively due to shorter escape times. We have modelled diffuse emissions at hundreds of TeV, relevant for measurements by LHAASO, Tibet AS-gamma, IceCube, and the upcoming SWGO, as well as at tens of GeV, as measured by Fermi-LAT. This reveals the distinctive nature of diffuse emissions at the respective energies which can likely be used to constrain source models and locate cosmic ray sources.

G. Lacedelli, E. Pallé, R. Luque, K. Ikuta, H.M. Tabernero, M.R. Zapatero Osorio, J.M. Almenara, F.J. Pozuelos, D. Jankowski, N. Narita, A. Fukui, G. Nowak, H.T. Ishikawa, T. Kimura, Y. Hori, K.A. Collins, S.B. Howell, C. Jiang, F. Murgas, H.P. Osborn, N. Astudillo-Defru, X. Bonfils, D. Charbonneau, M. Fausnaugh, S. Geraldía-González, K. Goździewski, P. Guerra, Y. Hayashi, K. Hodapp, K. Horne, K. Isogai, M. Jafariyazani, T. Kagetani, Y. Kawai, K. Kawauchi, V. Krishnamurthy, T. Kudo, T. Kurokawa, M. Kuzuhara, M. Mori, J. Nishikawa, S.K. Nugroho, M. Omiya, R.P. Schwarz, R. Sefako, A. Shporer, G. Srdoc, H. Teng, N. Watanabe

Sub-Neptunes are absent in the Solar System, yet they are commonly found in our Galaxy. They challenge the internal structure models and prompt investigation on their formation, evolution, and atmospheres. We report the characterisation of new sub-Neptunes orbiting two similar M dwarfs, TOI-521 (T_eff=3544 K), and TOI-912 (T_eff=3572 K). Both stars host a candidate identified by TESS and are part of the THIRSTEE follow-up program, which aims at understanding the sub-Neptune population through precise characterisation studies on a population level. We analysed light curves, ground-based photometry and ESPRESSO, HARPS and IRD RVs to infer precise orbital and physical parameters. The two stars host nearly identical planets in terms of mass and radius. TOI-521 b is a transiting sub-Neptune in a 1.5-d orbit with radius and mass of R=1.98+/-0.14 R_e and M=5.3+/-1.0 M_e respectively. Moreover, we identified an additional candidate at 20.3 d, with a minimum mass of Msini=10.7+/-2.4 M_e currently not detected to transit. Similarly, TOI-912 b is a 4.7-d sub-Neptune with R=1.93+/-0.13 R_e and M=5.1+/-0.5 M_e. Interestingly, TOI-912 b likely has an unusually high eccentricity (e=0.58+/-0.02), and it is probably undergoing strong tidal dissipation. If such eccentricity is confirmed, it would make it one of the most eccentric sub-Neptunes known to date. TOI-521 b and TOI-912 b have very similar densities (4 g/cm^3) and they lie in the degenerate region of the mass-radius diagram where different compositions are plausible, including a volatile-rich composition, or a rocky core surrounded by a H-He envelope. Our sample supports the division of sub-Neptunes into two distinct populations divided by a density gap. Both planets are interesting targets for atmospheric follow-up in the context of understanding the temperature-atmospheric feature trend that starts to emerge thanks to JWST observations.

Simon C. O. Glover, Ralf S. Klessen

Population III (or Pop. III) stars, the first stellar generation built up from metal-free primordial gas, first started to form at redshifts z ~ 30. They formed primarily in small dark matter halos with masses of a few million solar masses. The cooling of the gas in these halos was dominated on all scales by molecular hydrogen. Current theoretical models indicate that Pop. III stars typically formed in small clusters with a logarithmically flat mass function due to widespread fragmentation in the protostellar accretion disks around these primordial stars. Massive Pop. III stars are thought to have played a pivotal role in shaping the early Universe, as their feedback regulates subsequent star formation, although the immediate effects of this feedback remain uncertain. Direct detection of Pop. III stars is challenging, but our chances of detecting at least a few Pop. III supernovae within the next decade are brighter. Indirect approaches based on stellar archaeology or gravitational wave detections offer promising constraints. Current observations suggest that most massive Pop. III stars ended their lives as core-collapse supernovae rather than pair-instability supernovae, offering insight into the initial mass function and evolutionary pathways of these primordial stars.

Lorentz invariance violation (LIV) can have multiple consequences on very-high energy gamma rays' emission, propagation, and detection, such as energy-dependent photon group velocity, photon instability, vacuum birefringence, and modified electromagnetic interaction. Depending on the underlying theoretical model, several of these effects can coexist. Nevertheless, in experimental tests of LIV, each effect is tested separately and independently. Here, we are performing a search for traces of several coexisting effects in a single analysis. We present our analysis method based on artificial neural networks and put our very first results in the context of experimental searches for LIV.

Maryvonne Gerin, Harvey Liszt, Belén Tercero, José Cernicharo

The chemical composition of diffuse interstellar clouds is not fully established. They host an active chemistry despite their relatively low density and the ubiquitous presence of far-UV radiation. To further explore the chemical composition of diffuse clouds, we performed a spectral scan toward the bright radio source BL Lac in the Q band (from 32 to 50 GHz) using the Yebes 40m telescope. Yebes observations were performed interleaving Frequency Switching and Position Switching integrations toward BL Lac, using a spectral resolution of 38 kHz. The data have been reduced with the CLASS software. We achieved an unprecedented sensitivity on the continuum of 0.02 - 0.07 %, allowing the detection of very faint absorption features. We confirm previous detections of HCS+, C3H, C3H+, CH3CN and HC3N in diffuse clouds and report new detections of CCS, C4H, CH3CHO, H2CCO , HNCO and H2CS along the line of sight to BL Lac, with abundances relative to H2 from a few 10{-11} to a few 10{-10}. We compiled molecular detections toward diffuse clouds to obtain the chemical inventory of a typical diffuse interstellar cloud. The chemical inventory of diffuse interstellar clouds includes complex organic species with up to four heavy atoms. These species are efficiently formed in the diffuse interstellar gas and reach abundances similar to those measured in dense photodissociation regions, pointing to similar gas phase chemical processes.

We present a scalar-field formulation of the generalized Chaplygin gas (GCG) and modified Chaplygin gas (MCG) models, in which the cosmic fluid dynamics are reproduced by canonical Lagrangians with analytically derived energy density $\rho(\phi)$, pressure $p(\phi)$, and scalar potential $V(\phi)$. This framework provides a unified description of dark matter and dark energy, transitioning naturally from a matter-dominated phase at early times to a negative-pressure dark-energy phase at late times. In this scalar-field formulation, the GCG and MCG models are naturally applicable to both theoretical analyses and numerical simulations. Extending this approach, we develop a systematic method to obtain a class of integrable scalar-field cosmological models. In this study, we use this method to construct a new scalar-field altered Chaplygin gas (ACG) model. To investigate the viability of Chaplygin-type models, we perform a likelihood analysis using the Pantheon+ Type Ia supernova compilation together with Cepheid-calibrated distances. We examine four models, $\Lambda$CDM, GCG, MCG, and ACG, obtaining posterior constraints on the Hubble constant $H_0$, the present-day effective equation of state $\omega_0$, the transition redshift $z^\star$, and the cosmic age $t_0$. With the Cepheid calibration fixing the absolute distance scale, the inferred $H_{0}$ remains nearly model-independent. The Chaplygin-type models predict an earlier onset of cosmic acceleration than $\Lambda$CDM and give a broader range for the inferred age of the Universe, reflecting their greater flexibility in late-time expansion histories. Among them, the ACG model provides tighter parameter constraints, while the GCG and MCG models produce broader posteriors due to parameter degeneracies.

Supernova remnants (SNRs) are widely recognized as key accelerators of Galactic cosmic rays (CRs), supported by the detection of the characteristic pion bump in the gamma-ray spectra of several SNRs. However, the recent observation of ultra-high-energy (UHE, greater than 100 TeV) gamma-rays by LHAASO from sources such as W51 region challenges standard models, which predict CR acceleration up to PeV energies only during the early (~ 100 year) phase of SNR evolution. Given the older age of known SNRs, alternative mechanisms - such as the interaction of runaway CRs with nearby molecular clouds (MCs) - have been proposed to explain the persistent UHE emission. In this study, we focus on the W51 complex, particularly the W51C-B region, as a promising site for investigating SNR-MC interactions. Simulated observations with the CTAO and the ASTRI Mini-Array are presented to demonstrate their crucial role in bridging the energy gap between Fermi-LAT and LHAASO, especially in the 0.3-100 TeV range. Their improved angular resolution will also help disentangle emission components from the interaction zone and nearby sources. Our theoretical modelling suggests that accelerated particles at the shock can account for the radio and GeV data, while UHE emission could be best explained by the combined contribution from both acceleration and adiabatic compression of cloud material at the SNR-MC interface.

Characterizing the geometry of an object orbiting around a star from its transit light curve is a powerful tool to uncover various complex phenomena. This problem is inherently ill-posed, since similar or identical light curves can be produced by multiple different shapes. In this study, we investigate the extent to which the features of a shape can be embedded in a transit light curve. We generate a library of two-dimensional random shapes and simulate their transit light curves with light curve simulator, Yuti. Each shape is decomposed into a series of elliptical components expressed in the form of Fourier coefficients that adds increasingly diminishing perturbations to an ideal ellipse. We train deep neural networks to predict these Fourier coefficients directly from simulated light curves. Our results demonstrate that the neural network can successfully reconstruct the low-order ellipses, which describe overall shape, orientation and large-scale perturbations. For higher order ellipses the scale is successfully determined but the inference of eccentricity and orientation is limited, demonstrating the extent of shape information in the light curve. We explore the impact of non-convex shape features in reconstruction, and show its dependence on shape orientation. The level of reconstruction achieved by the neural network underscores the utility of using light curves as a means to extract geometric information from transiting systems.

O. Adriani (2 and 1), A. Albert (3 and 56), A. R. Alhebsi (4), S. Alshalloudi (4), M. Alshamsi (5), S. Alves Garre (6), A. Ambrosone (8 and 7), F. Ameli (9), M. Andre (10), L. Aphecetche (11), M. Ardid (12), S. Ardid (12), J. Aublin (13), F. Badaracco (15 and 14), L. Bailly-Salins (16), B. Baret (13), A. Bariego-Quintana (6), Y. Becherini (13), M. Bendahman (7), F. Benfenati Gualandi (18 and 17), M. Benhassi (19 and 7), D. M. Benoit (20), Beňušová (22 and 21), E. Berbee (23), E. Berti (2), V. Bertin (5), P. Betti (2), S. Biagi (24), M. Boettcher (25), D. Bonanno (24), S. Bottai (2), A. B. Bouasla (57), J. Boumaaza (26), M. Bouta (5), M. Bouwhuis (23), C. Bozza (27 and 7), R. M. Bozza (8 and 7), H.Brânzaš (28), F. Bretaudeau (11), M. Breuhaus (5), R. Bruijn (29 and 23), J. Brunner (5), R. Bruno (30), E. Buis (31 and 23), R. Buompane (19 and 7), J. Busto (5), B. Caiffi (15), D. Calvo (6), A. Capone (9 and 32), F. Carenini (18 and 17), V. Carretero (29 and 23), T. Cartraud (13), P. Castaldi (33 and 17), V. Cecchini (6), S. Celli (9 and 32), L. Cerisy (5), M. Chabab (34), A. Chen (35), S. Cherubini (36 and 24), T. Chiarusi (17), M. Circella (37), R. Clark (38), R. Cocimano (24), J. A. B. Coelho (13), A. Coleiro (13), A. Condorelli (13), R. Coniglione (24), P. Coyle (5), A. Creusot (13), G. Cuttone (24), R. Dallier (11), A. De Benedittis (19 and 7), G. De Wasseige (38), V. Decoene (11), P. Deguire (5), I. Del Rosso (18 and 17), L. S. Di Mauro (24), I. Di Palma (9 and 32), A. F. Díaz (39), D. Diego-Tortosa (24), C. Distefano (24), A. Domi (40), C. Donzaud (13), D. Dornic (5), E. Drakopoulou (41), D. Drouhin (3 and 56), J.-G. Ducoin (5), P. Duverne (13), R. Dvornický (22), T. Eberl (40), E. Eckerová (22 and 21), A. Eddymaoui (26), T. van Eeden (23), M. Eff (13), D. van Eijk (23), I. El Bojaddaini (42), S. El Hedri (13), S. El Mentawi (5), A. Enzenhöfer

Context: The detection of the highest energy neutrino observed to date by KM3NeT, with an estimated energy of 220 PeV, opens up new possibilities for the study and identification of the astrophysical sources responsible for a diffuse flux of such ultra-high-energy neutrinos, among which gamma-ray bursts are longstanding candidates. Aims: Based on the event KM3-230213A, we derive constraints on the baryon loading and density of the surrounding environment in models of blastwaves in long-duration gamma-ray bursts. Methods: We compute the diffuse flux from gamma-ray burst blastwaves, either expanding in a constant density interstellar medium or developing in a radially decreasing density of a wind-like environment surrounding the gamma-ray burst progenitor star, by taking into account the expected neutrino spectra and luminosity function. We use a Poisson likelihood method to constrain the blastwave model parameters by calculating the expected number of neutrino events within the 90% confidence level energy range of KM3-230213A and by using the joint exposure of KM3NeT/ARCA, IceCube and Pierre Auger. Results: We constrain the baryon loading to be $\leq \{392, 131, 39, 13\}$ at 90% confidence level, which is inversely proportional to a varying interstellar medium particle density of $\{1, 3, 10, 30\}$ cm$^{-3}$. In the wind-like environment case, the baryon loading is $\leq \{20, 50, 100\}$ at 90% confidence level, which is proportional to the sixth power of a varying density parameter of $\{0.05, 0.06, 0.07\}$.

This thesis explores experimental and theoretical approaches to dark matter detection, from gas-based detectors to quantum sensors, tackling the challenge of identifying dark matter, which makes up 27% of the Universe's energy. It reviews astrophysical and cosmological evidence, highlights the Standard Model's limitations, and motivates searches for WIMPs, axions, and dark photons through direct, indirect, and collider-based strategies. The experimental work includes the Micromegas-based TREX-DM experiment for low-mass WIMPs, with studies of argon and neon-based gas mixtures, detector design, shielding, readout, and background suppression. GEM integration boosted gain by up to 45. A UV LED-based internal calibration system was developed for compact, low-background operation, while pressure-dependent gain studies optimized future low-background TPCs. The thesis also advances axion and dark photon searches via haloscopes and introduces the DarkQuantum prototype, a superconducting qubit coupled to microwave cavities for single-photon detection. This system enabled the most stringent exclusion limit on massive dark photon interactions at 5.051 GHz, demonstrating the feasibility of quantum-enhanced detectors. Overall, the work bridges classical and quantum detection techniques, advancing WIMP searches and pioneering compact quantum sensors for axion and dark photon detection, laying the foundation for future high-sensitivity dark matter experiments.

Amina Boulkaboul, Lotfi Yelles Chaouche, Alessandro Carmelo Lanzafame, Yassine Damerdji

We present a spectroscopic and photometric study of HIP12653 to investigate its magnetic cycle and differential rotation. Using HARPS archival spectra matched with MARCS-AMBER theoretical templates, we derive the stellar parameters (Teff, logg, FeH, and vsini) of the target. The S-index, an activity indicator based on the emission of the CaII H&K lines, is fitted to determine the magnetic cycle and rotation periods. We refine the magnetic cycle period to 5799.20 \pm 0.88 d and suggest the existence of a secondary, shorter cycle of 674.6922 \pm 0.0098 d, making HIP12653 the youngest star known to exhibit such a short activity cycle. During the minimum activity phase, a rotation period of 4.8 d is estimated. This is notably different from the 7-day period obtained when measurements during minimum activity are excluded, suggesting that these two periods are rotation periods at different latitudes. To explore this hypothesis, we introduce a novel light curve fitting method that incorporates multiple harmonics to model different spot configurations. Applied to synthetic light curves, the method recovers at least two rotation periods close to the true input values in 92.1% of cases. The inferred rotation shear shows a median deviation of 0.0011 \pm 0.0003 and a standard deviation of 0.0177 \pm 0.0002 from the true value. Applying this approach to TESS photometric data from 2018 to 2023, we detect three distinct rotation periods, 4.8 d, 5.7 d, and 7.7 d, (along with a signal at 3.75 d interpreted as its first harmonic), consistent with spots located at different latitudes. Assuming a solar-like differential rotation, we estimate an inclination of 34.0 \pm 1.8^\circ and a rotational shear of \alpha = 0.38 \pm 0.01. These results confirm the 4.8-d period and demonstrate that differential rotation can be constrained by tracking rotation period changes across different phases of the magnetic cycle.

Performing a series of hydrodynamic stellar evolutionary simulations with \textsc{Mesa} (Module for Experiments in Stellar Astrophysics), we investigate the excitation and growth of radial pulsations of massive red supergiants (RSGs) with the initial mass range of $M_\mathrm{ini}=13$--$18\,\mathrm{M}_\odot$. We show that strong radial pulsations develop in the hydrogen-rich envelope in their late evolutionary stages, and eventually the surface radial velocity exceeds the escape velocity for higher-mass models. On the other hand, lower-mass models exhibit more moderate pulsations with finite velocity amplitudes and are expected to keep massive hydrogen-rich envelopes when they evolve toward the gravitational collapse of the iron core. While the latter group ends up as a familiar transient population of exploding RSGs, i.e., type IIP supernovae (SNe), the former group may expel a part of their envelopes and explode as different transients population. We investigate how the energy of the oscillating envelope is dissipated and released as radiation. We also empirically determine the condition for the pulsation-driven mass ejection in terms of the luminosity-to-mass ratio, $L/M>10^{3.9}\mathrm{L}_\odot/\mathrm{M}_\odot$. The corresponding luminosity threshold for the explored mass range may explain the observationally inferred constraints on type IIP SN progenitors.

Katja Fahrion, Michael A. Beasley, Anastasia Gvozdenko, Glenn van de Ven, Katherine L. Rhode, Ana L. Chies-Santos, Anna Ferre-Mateu, Marina Rejkuba, Oliver Müller, Eric Emsellem

Globular clusters (GCs) are dense star clusters found in all massive galaxies. Recent work has established that they follow a tight relation between their internal stellar velocity dispersion $\sigma$ and luminosity, enabling accurate distance measurements. In this work, we aim to apply this GC velocity dispersion (GCVD) distance method to measure the distance to M 104 (NGC 4594, the Sombrero galaxy). We have measured internal stellar velocity dispersions for 85 globular clusters (GCs) and one ultra-compact dwarf galaxy around M 104 using high-resolution multi-object integrated-light spectroscopy with FLAMES/GIRAFFE on the Very Large Telescope. The measured velocity dispersions range from $\sigma = 4 - 30$ km s$^{-1}$, with a mean uncertainty of $\Delta\sigma = 2.5$ km s$^{-1}$. For a subset of 77 GCs with $V$-band magnitudes and reliable velocity dispersion measurements above $\sigma > 4$ km s$^{-1}$, we constructed the $M_V$-$\sigma$ relation to measure the distance to M 104, finding $D=9.00\pm0.29$ (stat.) $\pm0.26$ (sys.) Mpc. The GCs follow the Milky Way and M 31 $M_V-\sigma$ relation closely, with the exception of the luminous ultra-compact dwarf SUCD1, which is nearly one magnitude brighter than the mean relation. 29 GCs in the sample have sizes determined from Hubble Space Telescope imaging which allowed us to determine their masses and $V$-band dynamical mass-to-light ratios (M/L$_V$). We find a mean $<M/L_V> = 2.6 \pm 0.8 M_{\odot}/L_{\odot}$ for the luminous ($M_V < -8$ mag) M 104 GCs, which is higher than the Milky Way GCs, but is reminiscent of the brightest GCs in Centaurus A. With the exception of SUCD1, the GCs of M 104 follow the GCVD relation irrespective of their mass-to-light ratio.

The Pierre Auger Observatory has recently undergone a major upgrade, called AugerPrime, tailored to answer the current most pressing questions in the ultra-high-energy cosmic ray (UHECR) detection. The AugerPrime upgrade consists of the addition, on top of each station, of a scintillator detector, to separate the muonic and electromagnetic component of the shower for better primary identification, and of a radio detector to measure the emission of air showers in 30-80 MHz range. An additional small diameter photomultiplier is installed in each station to increase the dynamic range for signal detection. New electronic modules, installed on all stations, provide a sufficient number of channels for the readout of the additional detectors, as well as faster sampling, increased dynamic range and processing capability. In this contribution we summarize the performance of the new electronic modules with respect to the requirements, describe the verification procedure and give the results in the laboratory tests compared to the performance in the field.

T. Miener, I. Viale, B. Lacave, A. Cerviño (for the CTAO-LST project)

The Cherenkov Telescope Array Observatory (CTAO), a next-generation ground-based gamma-ray observatory, will be composed of two arrays of multiple imaging atmospheric Cherenkov telescopes (IACTs) located in both the Northern and Southern Hemispheres. Its goal is to enhance the sensitivity of current instruments by a factor of five to ten over an energy range from 20 GeV to over 300 TeV. IACT arrays are used to probe the very-high-energy (VHE) gamma-ray sky, operating by simultaneously observing air showers triggered by the interaction of VHE gamma rays and cosmic rays with the atmosphere. Cherenkov photons produced by these showers create a stereoscopic record of the event. By reconstructing the event using machine learning techniques, the properties of the originating VHE particle-including its type, energy, and incoming direction-can be determined. In this contribution, we present a fully deep-learning-driven approach to reconstruct simulated, stereoscopic IACT events using CTLearn. CTLearn is a package designed for loading and manipulating IACT data and for running deep learning models with pixel-wise camera data as input.

P. Cox, K. M. Butler, C. R. Keeton, L. Eid, E. Borsato, T. J. L. C. Bakx, R. Neri, B. M. Jones, P. Prajapati, A. J. Baker, S. Berta, A. Cooray, E. M. Corsini, L. Marchetti, A. Omont, A. Beelen, R. Gavazzi, D. Ismail, R. J. Ivison, M. Krips, M.D. Lehnert, H. Messias, D. Riechers, C. Vlahakis, A. Weiß, P. van der Werf, C. Yang

We present a study of HerS-3, a dusty star-forming galaxy at zspec = 3.0607, which is gravitationally amplified into an Einstein cross with a fifth image of the background galaxy seen at the center of the cross. Detailed 1-mm spectroscopy and imaging with NOEMA and ALMA resolve the individual images and show that each of the five images display a series of molecular lines that have similar central velocities, unambiguously confirming that they have identical redshifts. The HST F110W image reveals a foreground lensing group of four galaxies with a photometric redshift zphot~1.0. Lens models that only include the four visible galaxies are unable to reproduce the properties of HerS-3. By adding a fifth massive component, lying south-east of the brightest galaxy of the group, the source reconstruction is able to match the peak emission, shape and orientation for each of the five images. The fact that no galaxy is detected near that position indicates the presence of a massive dark matter halo in the lensing galaxy group. In the source plane, HerS-3 appears as an infrared luminous starburst galaxy seen nearly edge-on. The serendipitous discovery of this exceptional Einstein cross offers a potential laboratory for exploring at small spatial scales a nuclear starburst at the peak of cosmic evolution and studying the properties of a massive dark matter halo associated with the lensing galaxy group.

Claims of anisotropy in the Hubble constant have been made based on direct distance tracers such as Tully-Fisher galaxies and Type Ia supernovae. We revisit these using the CosmicFlows-4 Tully-Fisher W1 subsample, 2MTF and SFI++ Tully-Fisher catalogues, and the Pantheon+ supernova compilation (restricted to $z < 0.05$), including a dipole in either the Tully-Fisher zero-point or the standardised supernova absolute magnitude. Our forward-modelling framework jointly calibrates the distance relation, marginalises over distances, and accounts for peculiar velocities using a linear-theory reconstruction. We compare the anisotropic and isotropic model using the Bayesian evidence. In the CosmicFlows-4 sample, we infer a zero-point dipole of amplitude $0.087 \pm 0.019$ mag, or $4.1\pm0.9$ per cent when expressed as a dipole in the Hubble parameter. This is consistent with previous estimates but at higher significance: model comparison yields odds of $877\!:\!1$ in favour of including the zero-point dipole. In Pantheon+ we infer zero-point dipole amplitude of $0.049 \pm 0.013$ mag, or $2.3\pm 0.6$ per cent when expressed as a dipole in the Hubble parameter. However, by allowing for a radially varying velocity dipole, we show that the anisotropic model captures local flow features (or possibly systematics) in the data rather than an actual linearly growing effective bulk flow caused by anisotropy in the zero-point or expansion rate. Inferring a more general bulk flow curve we find results fully consistent with expectations from the standard cosmological model.

Early stages of stellar birth comprise of a two-step process involving the formation of two hydrostatic cores. The second step of gravitational collapse sets the radiative efficiency and accretion rate of the young protostar. These two parameters, of prime importance for protostellar evolution, dictate the luminosities and thus play a key role in deciphering the current discrepancy between observational surveys and theoretical models. In this letter, we provide quantitative estimates on the evolution of the radiative efficiency and accretion rate obtained from self-consistent, high-resolution, radiative hydrodynamic simulations performed using the codes PLUTO and RAMSES. The main highlight of our result is that the radiative efficiency reaches unity, that is, supercriticality, relatively quickly after protostellar birth. Supercriticality at the accretion shock is a necessary condition for cold accretion. Our results thus support a rapid transition to the cold accretion scenario, which is one of the assumptions used in Pre-Main Sequence (PMS) models working towards solutions to explain observational data. We briefly discuss the implications of the time evolution of the radiative efficiency factor in the context of the luminosity problem, the Protostellar Luminosity Function (PLF), PMS evolution, accurate sink properties, and the stellar Initial Mass Function (IMF).

T. Miener, L. Burmistrov, B. Lacave, A. Cerviño (for the CTAO-LST project)

Imaging atmospheric Cherenkov telescopes (IACTs) detect extended air showers (EASs) generated when very-high-energy (VHE) gamma rays or cosmic rays interact with the Earth's atmosphere. Cherenkov photons produced during an EAS are captured by fast-imaging cameras, which record both the spatial and temporal development of the shower, along with calorimetric data. By analyzing these recordings, the properties of the original VHE particle-such as its type, energy, and direction of arrival-can be reconstructed through machine learning techniques. This contribution focuses on the Large-Sized Telescopes (LSTs) of the Cherenkov Telescope Array Observatory, a next-generation ground-based gamma-ray observatory. LSTs are responsible for reconstructing lower-energy gamma rays in the tens of GeV range. We explore a novel event reconstruction technique based on deep convolutional neural networks (CNNs) applied on calibrated and cleaned waveforms of the IACT camera pixels using CTLearn. Our approach explicitly incorporates the time development of the shower, enabling a more accurate reconstruction of the event. This method eliminates the need for charge integration or handcrafted feature extraction, allowing the model to directly learn from waveform data.

Duncan J. Bowden, Nandini Sahu, Anowar J. Shajib, Kim-Vy Tran, Tania M. Barone, Keerthi Vasan G.C., Daniel J. Ballard, Thomas E. Collett, Faith Dalessandro, Giovanni Ferrami, Karl Glazebrook, William J. Gottemoller, Leena Iwamoto, Tucker Jones, Glenn G. Kacprzak, Geraint F. Lewis, Haven McIntosh-Lombardo, Hannah Skobe, Sherry H. Suyu, Sarah M. Sweet

Double-source-plane strong gravitational lenses (DSPLs), with two sources at different redshifts, are independent cosmological probes of the dark energy equation of state parameter $w$ and the matter density parameter $\Omega_{\rm m}$. We present the lens model for the DSPL AGEL035346$-$170639 and infer cosmological constraints from this system for flat $\Lambda$CDM and flat $w$CDM cosmologies. From the joint posterior of $w$ and $\Omega_{\rm m}$ in the flat $w$CDM cosmology, we extract the following median values and 1$\sigma$ uncertainties: $w = -1.52^{+0.49}_{-0.33}$ and $\Omega_{\rm m} = 0.192^{+0.305}_{-0.131}$ from AGEL0353 alone. Combining our measurements with two previously analyzed DSPLs, we present the joint constraint on these parameters from a sample of three, the largest galaxy-scale DSPL sample used for cosmological measurement to date. The combined precision of $w$ from three DSPLs is higher by 15% over AGEL0353 alone. Combining DSPL and cosmic microwave background (CMB) measurements improves the precision of $w$ from CMB-only constraints by 39%, demonstrating the complementarity of DSPLs with the CMB. Despite their promising constraining power, DSPLs are limited by sample size, with only a handful discovered so far. Although ongoing and near-future wide-area sky surveys will increase the number of known DSPLs by up to two orders of magnitude, these systems will still require dedicated high-resolution imaging and spectroscopic follow-ups like those presented in this paper. Our ASTRO 3D Galaxy Evolution with Lenses (AGEL) collaboration is undertaking such follow-up campaigns for several newly discovered DSPLs and will provide cosmological measurements from larger samples of DSPLs in the future.

Yunliang Ren, Xiaofeng Yang, Xuwei Zhang, Shuangnan Chen, Yangjun Shi, Cheng Cheng, Xiaolong He, Hoernisa Iminniyaz

Coasting cosmology offers an intriguing and straightforward framework for understanding the universe. In this work, we employ the Trans-Planckian Censorship Criterion (TCC) conjecture to test the viability of the coasting cosmology and propose an entropic dark energy (EDE) model within this framework. By applying the holographic principle to constrain the dark energy density and adopting the Bekenstein entropy and Tsallis entropy as the constraining entropies of the system, we find that, in a holographic coasting cosmological framework where dark energy and dark matter evolve independently, the Tsallis entropy satisfies certain general assumptions better than the Bekenstein entropy. Thus, there may be a fundamental relationship between Tsallis entropy and dark energy. We utilize observational data from Type Ia Supernovae (SNIa), Baryon Acoustic Oscillations (BAO), and Cosmic Chronometers (CC) to constrain EDE model. The optimal Tsallis parameter obtained aligns well with theoretical expectations. To evaluate the model's fit to the observed data, we calculate the Akaike Information Criterion (AIC), Bayesian Information Criterion (BIC), and Kullback Information Criterion (KIC), and compare these metrics with those derived from $\Lambda$CDM, under which the model shows some improvement. Overall, this model provides a novel and simple on the evolution of the universe.

Sergey A. Belov, Yu Zhong, Dmitrii Y. Kolotkov, Valery M. Nakariakov

A hybrid machine learning model which combines a shallow convolutional neural network and a long short-term memory network (CNN--LSTM), has been developed to automate the detection of kink oscillations in coronal plasma loops within large volumes of high-cadence sequences of imaging data. The network was trained on a set of 10,000 synthetic data cubes designed to mimic sequences of coronal images, achieving an accuracy greater than 98\% on this synthetic dataset. The model was then applied to detect kink oscillations in real data cubes of coronal active regions observed with SDO/AIA in the 171~Å channel. This dataset consisted of 50 samples with visually detected kink oscillations and 128 samples without. Each sample covered an area of 260$\times$260~pixels in the spatial domain and a duration of 30~min with a 12~s cadence in the time domain. Both off-limb and on-disk regions of interest were used. The data were pre-processed by median filtering in the time domain, and Gaussian smoothing and Contrast Limited Adaptive Histogram Equalization in the spatial domain. In the real dataset, the performance of the model was 83.7\%.The model is fully available in open access. We regard the CNN--LSTM model developed as a first step toward creating robust tools for routine solar coronal data mining in the context of coronal oscillation study.

Nancy Remage Evans, Charles Proffitt, Pierre Kervella, Joanna Kuraszkiewicz, H. Moritz Günther, Richard I. Anderson, Alexandre Gallenne, Antoine Mérand, Boris Trahin, Giordano Viviani, Shreeya Shetye

V659 Cen is a classical Cepheid which is part of a multiple system. Previous observations have shown that a hot companion dominates an ultraviolet spectrum and a cooler main sequence star dominates an XMM-Newton spectrum. The Hubble Space Telescope (HST) Space Telescope Imaging Spectrograph (STIS) spectra discussed here spatially resolve the components and show that the secondary in the spectroscopic binary with the Cepheid is the low mass star, and the hottest star in the system is the outer companion. In addition a fourth star is a likely member of the system based on Gaia data. A new orbit is derived which includes new radial velocities.

We present updated constraints on an interacting dark energy - dark matter model with pure momentum transfer, where dark energy is in the form of a quintessence scalar field with an exponential potential. We run a suite of MCMC analyses using the DESI DR2 BAO measurements, in combination with CMB data from Planck and supernovae data from DESY5. In contrast to the standard case of uncoupled quintessence, we find that values for the potential's slope parameter $\lambda \geq \sqrt{2}$, which are conjectured by string theory scenarios, are not excluded. If $\lambda$ is fixed to such a value, we find that the data favour the negative coupling branch of the model, which is the branch exhibiting late-time growth suppression. We also derive 95% upper limits on the sum of the neutrino masses, finding $\sum m_\nu < 0.06$ eV ($\sum m_\nu < 0.16$ eV) when $\lambda$ is fixed (varied). Our results motivate further studies on dynamical dark energy models that obey string theory bounds and can be constrained with cosmological observations.

Anastasiia Mikhno, Federica Bradascio, Jonathan Biteau, François Brun, Patrick Brun, Hossam Boutalha, Justine Devin, Armelle Jardin-Blicq, Pierre Jean, Michael Josselin, Jean-Philippe Lenain, Quentin Luce, Vincent Marandon, Kevin Pressard, Georges Vasileiadis, CTAO NectarCAM Collaboration

The NectarCAM flat-field flasher is a calibration device designed for the camera that will equip the Medium-Sized Telescopes (MSTs) of the northern site of the Cherenkov Telescope Array Observatory (CTAO). Positioned in the centre of the MST dish, 16 meters in front of the camera, the flasher emits short (FWHM $\approx$ 5 ns), uniform (2$-$4%) light pulses to illuminate the entire focal plane. Accurate calibration is crucial for the optimal operation of the NectarCAM, ensuring precise gain computation and mitigating differences in light-collection efficiency of the pixels of the camera. Using the flat-field flasher, two informations are obtained : the pixel gain and the relative efficiency between pixels. In addition, the flasher is used to probe the dynamic range over which the camera operates effectively. In this study, we report on the performance characterisation of the flat-field flasher using a dedicated test bench. We report on the results of tests conducted on several flasher units, evaluating their reliability. Furthermore, we describe how the flat-field coefficients are applied within the camera to ensure uniformity of response of few percent level across all 1855 pixels. As the deployment of the first MST at the CTAO northern site is scheduled for 2027, this work represents a significant contribution to the collaboration`s efforts to finalize camera calibration systems.

J. M. Boxelaar, F. De Gasperin, M. J. Hardcastle, J. H. Croston, L. K. Morabito, R. J. van Weeren, H. Edler

The Low Frequency Array (LOFAR) is uniquely able to perform deep, 15" resolutions imaging at frequencies below 100 MHz. Observations in this regime, using the Low Band Antenna (LBA) system, are significantly affected by instrumental and ionospheric distortions. Recent developments in calibration techniques have enabled routine production of high-fidelity images at these challenging frequencies. The aim of this paper is to obtain images of the radio sources included in the Third Cambridge catalog, second revised version (3CRR), at an observing frequency of 58 MHz, with an angular resolution of 15"and sensitivity to both compact and diffuse radio emission. This work also aims to produce accurate flux measurements for all sources. This dataset is designed to serve as a reference for low-frequency radio galaxy studies and future spectral aging analyses. We deliver 58. MHz radio images for the complete 3CRR sample including flux density measurements. We determined that the LBA has an accurate flux density scale with an average flux uncertainty of 10%. This is an important confirmation for any future works using the LOFAR LBA system. With these results we characterize the bright radio galaxy population with new high-resolution low-frequency images. We also provide high-resolution models of these sources which will be useful for calibrating future surveys. This legacy survey significantly expands the available high-resolution data at low frequencies and is the first fully imaged high-resolution sample at ultra low frequencies (< 100 MHz). It lays the foundation for future studies of radio galaxy physics, low-energy cosmic-ray populations, and the interplay between radio jets and their environments.

Pierre Marchand, Audrey Coutens, Jean-Christophe Loison, Valentine Wakelam, Antoine Espagnet, Fernando Cruz-Sáenz de Miera

Complex organic molecules (COMs) are thought to be the precursors of pre-biotic molecules and are observed in many protostellar sources. For this paper we studied the formation of COMs during star formation and their evolution in the midplane of the circumstellar disk up to the end of the Class I stage. We used the Analytical Protostellar Environment (APE) code to perform analytical simulations of star formation and the Nautilus code to model the chemical evolution. Most COMs mainly form during the collapse or in the disk, except the lightest (CH3CCH, C3H6, CH3OH, CH3CHO, CH3OCH3, C2H5OH, CH3CN, CH3NC, C2H3CN, and CH3SH), which are significantly inherited by the disk from the prestellar phase. Over the first 150 kyr of the disk, the abundances of several COMs in the midplane vary negligibly (e.g., CH3CCH, CH3OH, and CH3CN), while others experience a variation of one order of magnitude (e.g., C2H3CHO HOCH2CHO, and CH3COCH2OH). Changing physical conditions also have an impact on the abundance profiles of COMs in the disk, and their inheritance. For example, increasing the temperature of the molecular cloud from 10 K to 15 K significantly promotes the formation of COMs in the prestellar phase, notably c-C2H4O and N-bearing species. Conversely, increasing the cloud mass from 2 Msol to 5 Msol only has a minor effect on the disk abundances in the early stages.

Timour Jestin, Thinh Nguyen, Laurent Eyer, Lorenzo Rimoldini, Ashish Mahabal, Marc Audard, Pedro Garcia-Lario, Panagiotis Gavras, Krzysztof Nienartowicz

The publications of Gaia DR2 and DR3 have brought major improvements in stellar astrometry and photometry, particularly regarding the description of the white dwarf sequence. Notably, Gaia DR2 enabled the detection of variability in white dwarfs based solely on averaged astrometric and photometric quantities, i.e. the astrometric 5 parameters (positions, proper motion, and parallax) and general photometry properties in the G, BP and RP bands (mean, standard deviation and number of measurements). We identify and classify variable white dwarfs using Gaia DR3 data and Zwicky Transient Facility DR23 observations. The objective is to construct a catalogue of pulsating white dwarf candidates with robust selection criteria. We define a new sample of candidate variable white dwarfs using Gaia DR3 astrometric and photometric data. We cross-match this sample with the ZTF DR23 catalogue and apply a multiband Lomb-Scargle periodogram analysis to detect periodic variability. We then use the OPTICS unsupervised clustering algorithm to to group and classify the confirmed periodic stars. We identify 1423 variable white dwarfs candidates from Gaia DR3, with 864 having ZTF time series. 141 present significant periodicity. We classify these objects into known categories, including ZZ Ceti stars, GW Vir, V777 Her, and white dwarf-main sequence binaries. Our analysis yields several periodic stars, including three ZZ Ceti, 15 GW Vir, one V777 Her, and 24 WD-MS binaries. Furthermore, it reveals a significant population of potentialy variable stars, though without confirmed periodicity. Finally we publish our catalogue of candidate variable white dwarfs including variability status, periodicity, and classification information for the 864 sources with ZTF time series, 519 of them newly identified (including 83 new periodic stars).

An alternative dark energy description based on a generalized K-essence scenario is here explored. In particular, we consider a \emph{quasi-quintessence} and/or \emph{quasi-phantom} field, whose pressure does not depend on the kinetic energy, firstly discussed in the context of the cosmological constant problem. In so doing, we fix the background evolution and investigate the main observational signatures of its corresponding fluid-like representation. The corresponding scalar field can be parameterized independently from the potential form and without imposing the condition $\omega \sim -1$ used for quintessence and phantom fields. Additionally, we constrain the model parameters by performing Monte-Carlo Markov chain simulations through the adoption of the Metropolis-Hastings algorithm and perform separated analyses, employing different data catalogs. More precisely, as data sets we employ observational Hubble data, type Ia supernovae and the second data release from the DESI Collaboration, namely DESI DR2. We define a hierarchy among analyses and, precisely, in the first we adopt all three samples, while the second excludes the DESI data points, with the aim of facing its effect on corresponding bounds. Our findings suggest that the \emph{quasi-quintessence} scenario prefers Planck's value of the Hubble constant $H_0$, but suggesting that, when the DESI sample is excluded from our computations, $\omega_0$ enters the phantom regime, although still compatible at $1$-$\sigma$ confidence level with a cosmological constant. Remarkably, these results appear in tension than those found for a standard quintessence, explored within the context of the recent DESI release, likely indicating that the DESI data may furnish inconclusive results depending on the kind of scalar field involved into the computation.

Michela Rigoselli, Sarah Recchia, Alberto Bonollo, Silvia Crestan, Giada Peron, Andrea Giuliani, Sandro Mereghetti

In recent years, the number of known sources emitting very- and ultra-high-energy gamma-rays has increased significantly thanks to facilities such as LHAASO and HAWC. Many of the observed sources are still unidentified or poorly constrained due to the limited angular resolution of these instruments; however, it is now ascertained that approximately half of them have a pulsar in coincidence. Some of these unidentified extended sources may be the result of the diffusion of leptons accelerated by the pulsar itself or in its nebula to energies exceeding 50 TeV. This new class of sources, called TeV halos, is characterized by a peculiar radial profile that, if properly resolved, is key to distinguishing them from other TeV sources that are associated with a pulsar, such as supernova remnants and pulsar wind nebulae. In this contribution, we consider all the pulsars which are spatially coincident with an unidentified extended TeV source, in order to quantify whether its spin-down power, age and distance allow the pulsar to produce a TeV halo with the observed flux and extension. We also investigate how the next generation of Imaging Atmospheric Cherenkov Telescopes (IACTs), namely the Cherenkov Telescope Array Observatory (CTAO) and the ASTRI Mini-Array, will observe and characterize these TeV halos. We present a set of simulated sources with the expected morphology and spectrum, and we show for which of them we can distinguish between TeV halos and other classes of extended sources.

Radio interferometric imaging has long relied on the CLEAN algorithm, valued for its speed, robustness, and integration with calibration pipelines. However, next-generation facilities such as the ngVLA, SKA, and ALMAs Wideband Sensitivity Upgrade will produce data volumes and dynamic ranges that exceed the scalability of traditional methods. CLEAN remains dominant due to its simplicity and accumulated expertise, yet its assumption of modeling the sky as point sources limits its ability to recover extended emission and hampers automation. We review CLEANs limitations and survey alternatives, including multiscale extensions, compressive sensing, Regularized Maximum Likelihood, Bayesian inference, and AI-driven approaches. Forward-modeling methods enable higher fidelity, flexible priors, and uncertainty quantification, albeit at greater computational cost. Hybrid approaches such as Autocorr-CLEAN, CG-CLEAN, and PolyCLEAN retain CLEANs workflow while incorporating modern optimization. We argue hybrids are best suited for the near term, while Bayesian and AI-based frameworks represent the long-term future of interferometric imaging.

Arghyadeep Basu, Benedetta Ciardi, James S. Bolton, Matteo Viel, Enrico Garaldi

Interpreting Lyman-$\alpha$ forest properties during the epoch of reionization requires assumptions about the spectral energy distribution (SED) of ionizing sources. These are often simplified to blackbody or power-law spectra, potentially overlooking contributions from high-energy processes. In this work, we investigate how different SED models of reionization-era sources shape the thermal and ionization state of the intergalactic medium (IGM) and imprint on the Ly$\alpha$ forest during the late stages of reionization. We perform $3D$ radiative transfer simulations with CRASH, post-processed on Sherwood-type hydrodynamical outputs, exploring both physically motivated SEDs including X-ray binaries, Bremsstrahlung from shock-heated interstellar medium, and binary stars and idealized blackbody and power-law spectra. While the large-scale morphology of ionized regions is broadly similar across all models, harder spectral components extend partially ionized zones, produce larger He III regions, and heat the surrounding IGM. By adopting simplified spectra there is the risk of underestimating the contribution of high-energy sources, which subtly alter the effective optical depth, the flux power, and the local transmissivity, potentially biasing constraints on the thermal and ionization history of the IGM. The differences across models are most pronounced in the behavior of the proximity zone and in the power at intermediate scales, offering the most promising diagnostics to disentangle source populations. With upcoming high precision measurements from ELT and DESI, realistic SED modelling will be essential for robustly connecting Ly$\alpha$ forest observations to the sources driving the end of reionization.

We present a flexible, annulus-by-annulus method to constrain the 2-D thermal structure of a protoplanetary disk from optically thick spectral line emission. Using synthetic disk models with a known temperature and density structure, we extracted the vertical emission surfaces and brightness temperatures in radial annuli for multiple CO isotopologue transitions and used them to infer the vertical temperature profiles. This approach reliably recovers the injected temperature structure despite noise and finite resolution. We demonstrated that even a modest set of emission lines can constrain the temperature across a wide range of radii and elevations. Nevertheless, biases in the extracted emission surfaces constitute a major source of systematic error. Finally, we applied this method to archival ALMA observations of the HD 163296 disk, revealing that simple parametric radial temperature models may obscure the complexity of real disks and that additional observations are necessary to distinguish between different models of the vertical structure. This flexible framework can be readily applied to other systems, helping to characterize the thermal environments that shape planet formation.

During the final assembly of gas giant planets, circumplanetary disks (CPDs) of gas and dust form due to the conservation of angular momentum, providing material to be accreted onto the planet and the ingredients for moons. The composition of these disks has remained elusive, as their faint nature and short separations from their host stars have limited our ability to access them. Now, with the spatial and spectral resolution of JWST/MIRI Medium-Resolution Spectrograph, we can observe and characterize this reservoir for wide-orbit planetary-mass companions for the first time. We present the mid-infrared spectrum from the CPD surrounding the young companion CT Cha b. The data show a carbon-rich chemistry with seven carbon-bearing molecules (up to C$_6$H$_6$) and one isotopologue detected and indicate a high gaseous C/O$>$1 that is in contrast with the elemental abundance ratios typically measured in directly imaged gas giant atmospheres. This carbon-rich chemistry is also in stark contrast to the spectrum of the disk surrounding the host star, CT Cha A, which shows no carbon-bearing molecules. This difference in disk chemistry between the host disk and its companion indicates rapid, divergent chemical evolution on $\sim$million-year timescales. Nonetheless, the chemical properties of the CPD follow trends observed in isolated objects, where disks transition from an oxygen-rich to carbon-rich composition with decreasing host mass. Our results provide the first direct insight into the chemical and physical properties of material being accreted onto a gas giant analogue and into its potential moon system.

The peculiar velocities of dark matter tracers drive the growth of cosmic structures, providing a sensitive test of cosmological models and strengthening constraints on the nature of dark energy. In this work, we investigate the mean pairwise velocities, $v_{12}$, of dark matter tracers as a cosmological probe in the non-linear regime of cosmic structure formation. Using N-body dark matter-only simulations, we measure $v_{12}$ for pair separations up to 50 $h^{-1}$Mpc and model it by solving the pair conservation equation for a self-gravitating particle system, along with various prescriptions of the nonlinear matter power spectrum. We quantified the sensitivity of $v_{12}$ to variations in key cosmological parameters such as $\Omega_{\mathrm{m}}$, $\sigma_8$, $h$, $M_\nu$, and $w$. Our parameter inference analysis using MCMC shows sub-11% agreement with simulation data, with notable degeneracies, particularly between $\Omega_\mathrm{m}$ and $\sigma_8$. We further compute the stable clustering crossing scale across redshifts $z=0$, $0.5$, and $1$, assessing its dependence on cosmology. Among the tested power spectrum modeling approaches, we find that the CSSTEmu emulator provides the most accurate predictions, with deviations below 5% for $r > 10$ $h^{-1}$Mpc at $z=0.5$. Our results are validated using independent simulation suites, demonstrating that our framework offers a robust method for extracting cosmological constraints from upcoming peculiar velocity data.

We consider gravitational collapse of a fluid sphere with torsion generated by spin, which forms a black hole. We use the Tolman metric and the Einstein$-$Cartan field equations with a relativistic spin fluid as a source. We show that gravitational repulsion of torsion prevents a singularity, replacing it with a nonsingular bounce. Quantum particle creation during contraction prevents shear from overcoming torsion. Particle creation during expansion can generate a finite period of inflation and produce large amounts of matter. The resulting closed universe on the other side of the event horizon may have several bounces. Such a universe is oscillatory, with each cycle larger than the preceding cycle, until it reaches a size at which dark energy dominates and expands indefinitely. Our Universe might have therefore originated from a black hole existing in another universe.

We present a simplified review of inflationary cosmology across various modified gravity theories. These include models based on curvature, torsion, and non-metricity. We explore how scalar fields interact with different geometric quantities and how these interactions affect inflationary dynamics. Key cosmological features such as background evolution, reheating, and observable parameters are discussed. We also examine exotic scenarios inspired by string theory, extra dimensions, and non-local models. This work aims to connect theoretical models with observational data and future missions, offering guidance for exploring inflation beyond general relativity.

Jaanita Mehrani, Tao Xu, Andrey Baydin, Michael J. Manfra, Henry O. Everitt, Andrew J. Long, Kuver Sinha, Junichiro Kono, Shengxi Huang

We propose the Semiconductor-Quantum-Well Axion Radiometer Experiment ($\texttt{SQWARE}$) -- a new experimental platform for direct detection of axion dark matter in the meV mass range -- based on resonantly enhanced axion-photon conversion through the inverse Primakoff effect in engineered quantum semiconductor heterostructures. The core of the radiometer is a GaAs/AlGaAs multiple quantum well structure forming a magnetoplasmonic cavity, containing an ultrahigh-mobility two-dimensional electron gas, which realizes a tunable epsilon-near-zero resonance in the terahertz frequency range. By controlling the orientation of the cavity within a strong external magnetic field, both the resonance frequency and the axion-induced current are optimized $\textit{in situ}$, enabling efficient scanning across a broad mass range without complex mechanical adjustment. The axion-induced electromagnetic signal radiatively emitted from the magnetoplasmonic cavity is detected by a state-of-the-art photodetector. We present the theoretical basis for resonant enhancement, detail the experimental design and benchmarks through extensive simulations, and project the sensitivity of $\texttt{SQWARE}$ for several realistic configurations. Our results demonstrate that $\texttt{SQWARE}$ can probe the well-motivated quantum chromodynamics axion parameter space and close a critical gap in direct searches at meV masses.

We investigate a particle dark matter (DM) scenario where the DM interaction with the Standard Model are mediated by a leptophilic effective operator. Unlike conventional WIMP scenarios where thermal freeze-out occurs in a radiation-dominated Universe, we consider DM freeze-out during a prolonged reheating epoch driven by inflaton decay. The resulting departure from standard cosmology alters the thermal evolution of the dark matter abundance, making it sensitive to the reheating temperature and the history of entropy injection. The leptophilic nature of the interaction, motivated by the absence of DM signals in the current LHC searches, suppresses couplings to quarks and gluons and instead enables viable DM-lepton interactions that remain largely unconstrained. Within this setup, we analyze the mono-Higgs plus missing energy channel at future lepton colliders where the same operator responsible for setting the relic abundance can be directly probed. We perform a detailed signal-background analysis using both polarized and unpolarized beams. Additionally, our results illustrate how collider experiments, when interpreted jointly with relic density constraints, can provide indirect hints of the Universe's thermal history, offering potential insights into the reheating temperature and the dynamics preceding Big Bang Nucleosynthesis.

Initial Orbit Determination (IOD) is the classical problem of estimating the orbit of a body in space without any presumed information about the orbit. The geometric formulation of the ''angles-only'' IOD in three-dimensional space: find a conic curve with a given focal point meeting the given lines of sight (LOS). We provide an algebraic reformulation of this problem and confirm that five is the minimal number of lines necessary to have a finite number of solutions in a non-special case, and the number of complex solutions is 66. We construct a subdivision method to search for the normal direction to the orbital plane as a point on the real projective plane. The resulting algorithm is fast as it discovers only a handful of the solutions that are real and physically meaningful.

The finite electron mass can cause magnetic reconnection even in the absence of any other non-ideal effect in a magnetic evolution. It will be shown that when electron inertia is the only non-ideal effect in the evolution of the magnetic field $\vec{B}$, there is a related field that evolves ideally. This field is $\vec{\mathcal{B}} \equiv \vec{B} + \vec{\nabla}\times \left( (m_e/n e^2) \vec{j} \right)$ with $m_e$ the electron mass, $n$ the electron number density, and $\vec{j}$ the current density. Although the magnetic field is modified from its ideal evolution form by the electron inertia, the effect on particle trajectories, even electron trajectories, is small unless the current lies in thin sheets, which make $\vec{j}$ extremely large. The field $\vec{\mathcal{B}}$ is closely related to Voigt normalized magnetic field, which is defined by a Laplacian smoothing of $\vec{B}$. The difference between $\vec{\mathcal{B}}$ and $\vec{B}$ involves the relativistically invariant four-space Laplacian acting on $\vec{B}$ with a $c/\omega_{pe}$ smoothing distance; $\omega_{pe}$ is the plasma frequency.

The plethora of space-borne and ground-based observatories has provided astrophysicists with an unprecedented volume of data, which can only be processed at scale using advanced computing algorithms. Consequently, ensuring the quality of data fed into machine learning (ML) models is critical. The H$\alpha$ observations from the GONG network represent one such data stream, producing several observations per minute, 24/7, since 2010. In this study, we introduce a lightweight (non-ML) anomaly-detection algorithm, called H-Alpha Anomalyzer, designed to identify anomalous observations based on user-defined criteria. Unlike many black-box algorithms, our approach highlights exactly which regions triggered the anomaly flag and quantifies the corresponding anomaly likelihood. For our comparative analysis, we also created and released a dataset of 2,000 observations, equally divided between anomalous and non-anomalous cases. Our results demonstrate that the proposed model not only outperforms existing methods but also provides explainability, enabling qualitative evaluation by domain experts.

We present a comprehensive evaluation of the nuclear structure properties of 19Ne using a novel and rigorous Bayesian statistical framework. Precise characterization of 19Ne resonance parameters is critical for accurately determining reaction rates of the astrophysically significant 15O(alpha, gamma)19Ne and 18F(p, alpha)15O reactions, which govern breakout from the hot CNO cycle in X-ray bursts and influence gamma-ray emission in novae, respectively. By reconstructing likelihood functions from published experimental data, including asymmetric uncertainties and upper or lower limits, we derive posterior distributions for resonance energies, decay widths, and branching ratios. Our Bayesian approach systematically incorporates previously reported discrepancies among measurements, providing a statistically robust and consistent treatment of these uncertainties. The evaluated resonance parameters and associated uncertainties provide crucial input for stellar nucleosynthesis modeling, contributing to a refined understanding of explosive astrophysical phenomena.

We derive generalized geodesic equations in curved spacetime that include conservative forces, dissipative effects, and quantum-gravity-motivated minimal-length corrections. Conservative interactions are incorporated through external vector potentials, while dissipative dynamics arise from an exponential rescaling of the particle Lagrangian. Quantum-gravity effects are introduced via Generalized Uncertainty Principle (GUP) deformed Poisson brackets in the Hamiltonian framework. We show that free-particle geodesics remain unaffected at leading order, but external potentials induce velocity-dependent corrections, implying possible violations of the equivalence principle. As an application, we analyze modified trajectories in Friedmann-Lemaitre-Robertson-Walker (FLRW) universes dominated by dust, radiation, stiff matter, and dark energy. Our results establish a unified approach to conservative, dissipative, and GUP-corrected geodesics, providing a framework to probe the interplay between external forces, spacetime curvature, and Planck-scale physics.

We investigate cosmology-driven modifications to Schwarzschild-like black hole spacetimes and analyze their impact on photon propagation, gravitational lensing, and shadow observation. The gravitational deflection angle is computed using the Rindler-Ishak method, which incorporates finite-distance corrections and provides a consistent framework for non-asym-ptotically flat spacetimes. The effective potential for null geodesics exhibits a single unstable maximum corresponding to the photon sphere, and we study photon orbits classified according to the critical impact parameter into capture, escape, and unstable circular trajectories. Our analysis shows that the deflection angle decreases with increasing model parameter $(\alpha)$, resulting in weaker light bending compared to the Schwarzschild case. In addition, we examine the angular diameter of the black hole shadow as measured by a static observer, highlighting its dependence on the cosmological modification parameters. These results suggest that high-precision astrometric and lensing observations can place meaningful constraints on cosmology-inspired modifications to gravity, thereby linking astrophysical black holes with cosmic expansion and offering a novel probe of gravitational physics in strong-field regimes.

We develop a theoretical framework for axion dark matter (DM) searches using terrestrial electromagnetic (EM) fields. Axions couple to the geomagnetic field and generate a monochromatic EM signal at a frequency set by the axion mass. Incorporating a realistic atmospheric conductivity, we describe the axion-induced EM waves confined in the Earth-ionosphere cavity, avoiding the divergences present in idealized treatments. Our semi-analytical method yields quantitative predictions for the axion-induced magnetic field near the Earth's surface, and we found that (i) at $m_{\rm a} \gtrsim 10^{-14}$ eV, the signal exhibits resonance structures aligned with Schumann resonances, and the magnetic field amplitude is especially enhanced at $m_{\rm a} \sim 3 \times 10^{-14}$ eV. (ii) The signal amplitude and orientation also vary with geographic location, with Southeast Asia offering the strongest sensitivity. These predictions are insensitive to uncertainties in conductivity models and boundary conditions. Those distinctive features provide a reliable template to distinguish axion-induced signals from natural or anthropogenic EM backgrounds, and the formalism can be extended to other DM candidates such as dark photons.

Weak interactions cause small parity-violating energy differences between left- and right-handed chiral systems. Although normally tiny, these effects may be significantly enhanced during collective phenomena such as phase transitions. We propose a theoretical model describing the enhancement of weak interactions in phase transitions. The enhancement factor is proportional to the critical number of atoms, $N_c$, in the nucleus of the new phase. After the nucleus reaches its critical size, it grows until it fills the entire system. Measurement of the ratio of produced left and right chiral structures may provide a way to measure this critical number $N_c$. Experiments where definite spin-chiral structures are formed during a phase transition in crossed electric and magnetic fields, indicate $N_c \sim 10^9 - 10^{10}$. An open question is whether a similar enhancement could operate during cosmological phase transitions - thereby boosting CP-violating effects sufficiently to contribute to the observed matter-antimatter asymmetry (baryogenesis).

J. Nippert, S. Courtin, M. Heine, D.G. Jenkins, P. Adsley, A. Bonhomme, R. Canavan, D. Curien, T. Dumont, E. Gregor, G. Harmant, E. Monpribat, L. Morrison, M. Moukaddam, M. Richer, M. Rudigier, J.G. Vega Romero, W.N. Catford, P. Cotte, S. Della Negra, G. Haefner, F. Hammache, J. Lesrel, S. Pascu, Zs. Podolyák, P.H. Regan, I. Ribaud, N. de Séréville, C. Stodel, J. Vesić

Purpose: We have investigated the cross section around the lowest direct coincident gamma-particle measurements, where previously only limits could be established with the aim of obtaining a detailed description of the excitation function. We have furthermore analysed the ratio of extreme decay branching into the first excited state of daughter nuclei with alpha or proton emission at relative kinetic energies where previous measurements are in disagreement with each other. Conclusions: Our findings in the astrophysics RoI support reaction-rate models with a lower average S-factor trend, that deviates significantly from standard extrapolations between 2.2 MeV and 2.6 MeV, for stellar carbon burning simulations of up to 25 Msol stars. Based on our data, an overall increase of the S-factor at deep subbarrier energy cannot be confirmed. The extremely low ratio of the branching into the first excited state with proton over alpha emission of ~ 2% at 3.23 MeV might indicate the presence of alpha cluster compound states in 24Mg. This highly favours {\alpha} emission with fundamental consequences in possible stellar carbon burning sites.

We construct the Lagrangian formulation of a micro-structured spinning, dilating and shearing (deformable) test body, moving in arbitrary non-Riemannian backgrounds possessing all geometrical entities of curvature, torsion and non-metricity. We start with a Lagrangian of a generic form that depends on the particle's velocity, its material frame and its absolute derivative, and the background geometry consisting of a metric and an independent affine connection. Performing variations of the path and the material frame, we derive the equations of motion for the particle that govern the evolution of its momentum and hypermomentum in this generic background. The reported equations of motion generalize those of a spinning particle (Mathisson \cite{Mathisson:1937zz}, Papapetrou \cite{Papapetrou:1951pa}, Dixon \cite{Dixon:1974xoz}) by the inclusion of the dilation and shear (hadronic) currents of matter. Using the derived equations of motion, a generalized conserved quantity is also found. Further conserved quantities that can be obtained by appropriate supplementary conditions are also discussed.

We present a comprehensive investigation of the F-statistic method for parameter estimation of gravitational wave (GW) signals from binary black hole mergers. By analytically maximizing the likelihood over the luminosity distance and polarization angle, this approach reduces the dimensionality of the parameter space to enhance computational efficiency. We also introduce a novel formulation for calculating the Bayes factor for the F-statistic, enabling a quantitative assessment of its performance against standard full frequency-domain (FFD) Bayesian inference. Using the benchmark event GW150914, we demonstrate that the F-statistic method is not only approximately $70\%$ faster than FFD but is also statistically stable across different sampler configurations, with a log-Bayes factor between runs smaller than $0.1$. Furthermore, the F-statistic exhibits superior stability against changes in sampler configuration, yielding consistently lower Jensen-Shannon divergence values between analysis runs. While the F-statistic produces slightly broader constraints on some parameters, we argue this represents a more honest uncertainty quantification, particularly in high-dimensional parameter spaces with complex posterior structures. These results highlight the significant advantages of the F-statistic method for GW data analysis, positioning it as a powerful tool for the era of high-rate detections with future observatories.

The velocity distribution of cold dark matter within galaxies is expected to exhibit ultra-fine-grained substructure as a result of the many foldings of an initially smooth phase-space sheet under gravity. The innumerable folds of this sheet in the inner regions of a galactic halo would appear on solar-system scales like an extremely large number of spatially overlapping streams of dark matter particles. Some of these streams may also receive amplified densities if dark matter undergoes enhanced clustering in the early Universe, as is the case for axions in the post-inflationary scenario. This ultra-fine-grained dark matter substructure is usually considered irrelevant and undetectable for most direct detection experiments, but for axion haloscopes, this may not be the case. We develop and explore several plausible models for the degree of fine-grained axion dark matter substructure so as to evaluate its impact on the detectability of axions. We find that not only is this substructure detectable in haloscope experiments, but that it may enhance the detectability of the axion if data is analysed with a high-enough frequency resolution. This conclusion motivates ongoing high-resolution analyses of axion data by haloscope collaborations, which have the potential to reveal evidence of the QCD axion even if their nominal experimental sensitivity does not reach the required level under the Standard Halo Model assumption.

We investigate the impact of shot noise on the stochastic gravitational wave background generated by binary neutron star mergers, and confirm that the overall background can be significantly influenced by relatively few neighboring, loud events. To mitigate the shot noise, we propose a procedure to remove nearby events by notching them out in the time-frequency domain. Additionally, we quantify the cosmic/sample variance of the resulting background after notching, and we study the deviation between the cross-correlation measurement and the theoretical prediction of the background. Taking both effects into account, we find that the resulting sensitivity loss in the search for an isotropic background formed by binary neutron star mergers is minimal, and is limited to $\lesssim 4\%$ below 40 Hz, and to $\lesssim 1\%$ above 40 Hz.

Arjun Berera, Heliudson Bernardo, Suddhasattwa Brahma, Jaime Calderón-Figueroa, Rudnei O. Ramos, Michael W. Toomey

In this paper we propose a two-field model of warm inflation motivated from a heterotic string construction. The model contains an axion and a dilaton-like field. We show that while warm inflation can take place in the axion-field direction, thermal corrections coming from the radiation gauge fields, which couples to both the axion and the dilaton, prevent warm inflation to happen in the dilaton-field direction. We explore the background dynamics for different parameters, and identify a diversity of dynamical behaviors allowed in this model, denoting different regimes of warm inflation.