30 results on '"fundamental parameters. [Galaxies]"'
Search Results
2. EAGLE-like simulation models do not solve the entropy core problem in groups and clusters of galaxies
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Edoardo Altamura, Scott T Kay, Richard G Bower, Matthieu Schaller, Yannick M Bahé, Joop Schaye, Josh Borrow, and Imogen Towler
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Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,FOS: Physical sciences ,numerical [methods] ,Astronomy and Astrophysics ,groups [galaxies] ,Astrophysics - Astrophysics of Galaxies ,simulations [software] ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,hydrodynamics ,clusters [galaxies] ,fundamental parameters [galaxies] ,intracluster medium [galaxies] ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
Recent high-resolution cosmological hydrodynamic simulations run with a variety of codes systematically predict large amounts of entropy in the intra-cluster medium at low redshift, leading to flat entropy profiles and a suppressed cool-core population. This prediction is at odds with X-ray observations of groups and clusters. We use a new implementation of the EAGLE galaxy formation model to investigate the sensitivity of the central entropy and the shape of the profiles to changes in the sub-grid model applied to a suite of zoom-in cosmological simulations of a group of mass $M_{500} = 8.8 \times 10^{12}~{\rm M}_\odot$ and a cluster of mass $2.9 \times 10^{14}~{\rm M}_\odot$. Using our reference model, calibrated to match the stellar mass function of field galaxies, we confirm that our simulated groups and clusters contain hot gas with too high entropy in their cores. Additional simulations run without artificial conduction, metal cooling or AGN feedback produce lower entropy levels but still fail to reproduce observed profiles. Conversely, the two objects run without supernova feedback show a significant entropy increase which can be attributed to excessive cooling and star formation. Varying the AGN heating temperature does not greatly affect the profile shape, but only the overall normalisation. Finally, we compared runs with four AGN heating schemes and obtained similar profiles, with the exception of bipolar AGN heating, which produces a higher and more uniform entropy distribution. Our study leaves open the question of whether the entropy core problem in simulations, and particularly the lack of power-law cool-core profiles, arise from incorrect physical assumptions, missing physical processes, or insufficient numerical resolution., Accepted for publication in MNRAS on 2023 February 06. The code used in the analysis is publicly available on the corresponding author's GitHub repository: https://github.com/edoaltamura/entropy-core-problem
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- 2023
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3. The LEGA-C and SAMI galaxy surveys: quiescent stellar populations and the mass–size plane across 6 Gyr
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Tania M Barone, Francesco D’Eugenio, Nicholas Scott, Matthew Colless, Sam P Vaughan, Arjen van der Wel, Amelia Fraser-McKelvie, Anna de Graaff, Jesse van de Sande, Po-Feng Wu(吳柏鋒), Rachel Bezanson, Sarah Brough, Eric Bell, Scott M Croom, Luca Cortese, Simon Driver, Anna R Gallazzi, Adam Muzzin, David Sobral, Joss Bland-Hawthorn, Julia J Bryant, Michael Goodwin, Jon S Lawrence, Nuria P F Lorente, and Matt S Owers
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statistics [galaxies] ,galaxies structure ,FOS: Physical sciences ,galaxies statistics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,SCALING RELATIONS ,SURVEY DATA RELEASE ,HIGH-REDSHIFT GALAXIES ,abundances [galaxies] ,TO-LIGHT RATIO ,fundamental parameters [galaxies] ,Astrophysics::Solar and Stellar Astrophysics ,INTEGRAL FIELD SPECTROSCOPY ,evolution [galaxies] ,Astrophysics::Galaxy Astrophysics ,STAR-FORMATION HISTORIES ,FORMING GALAXIES ,Astronomy and Astrophysics ,stellar content [galaxies] ,ATLAS(3D) PROJECT ,galaxies fundamental parameters ,Astrophysics - Astrophysics of Galaxies ,galaxies evolution ,Physics and Astronomy ,SURFACE-DENSITY ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,EVOLUTION DATABASE ,galaxies abundances ,structure [galaxies] ,galaxies stellar content - Abstract
We investigate the change in mean stellar population age and metallicity ([Z/H]) scaling relations for quiescent galaxies from intermediate redshift ($0.60\leq z\leq0.76$) using the LEGA-C Survey, to low redshift ($0.014\leq z\leq0.10$) using the SAMI Galaxy Survey. We find that, similarly to their low-redshift counterparts, the stellar metallicity of quiescent galaxies at $0.60\leq z\leq 0.76$ closely correlates with $M_*/R_\mathrm{e}$ (a proxy for the gravitational potential or escape velocity), in that galaxies with deeper potential wells are more metal-rich. This supports the hypothesis that the relation arises due to the gravitational potential regulating the retention of metals, by determining the escape velocity required by metal-rich stellar and supernova ejecta to escape the system and avoid being recycled into later stellar generations. On the other hand, we find no correlation between stellar age and $M_*/R_\mathrm{e}^2$ (stellar mass surface density $\Sigma$) in the LEGA-C sample, despite this being a strong relation at low redshift. We consider this change in the age--$\Sigma$ relation in the context of the redshift evolution of the star-forming and quiescent populations in the mass--size plane, and find our results can be explained as a consequence of galaxies forming more compactly at higher redshifts, and remaining compact throughout their evolution. Furthermore, galaxies appear to quench at a characteristic surface density that decreases with decreasing redshift. The $z\sim 0$ age--$\Sigma$ relation is therefore a result of building up the quiescent and star-forming populations with galaxies that formed at a range of redshifts and so a range of surface densities., Comment: 18 pages, 11 figures, accepted to MNRAS
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- 2022
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4. GOODS-ALMA 2.0: Last gigayear star formation histories of the so-called starbursts within the main sequence
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Ciesla, L, Gómez-Guijarro, C, Buat, V, Elbaz, D, Jin, S, Béthermin, M, Daddi, E, Franco, M, Inami, H, Magdis, G, Magnelli, B, Xiao, M, Laboratoire d'Astrophysique de Marseille (LAM), and Aix Marseille Université (AMU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)
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FORMING GALAXIES ,SUBMILLIMETER GALAXIES ,QUIESCENT ,FOS: Physical sciences ,MASSIVE GALAXIES ,Astronomy and Astrophysics ,HIGH-Z GALAXIES ,evolution [Galaxies] ,Astrophysics - Astrophysics of Galaxies ,EVOLUTION ,MODEL ,[SDU]Sciences of the Universe [physics] ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,fundamental parameters [Galaxies] ,STELLAR-MASS ,RECONSTRUCTION ,HIGH-REDSHIFT - Abstract
Recently, a population of compact main sequence (MS) galaxies exhibiting starburst-like properties have been identified in the GOODS-ALMA blind survey at 1.1mm. Several evolution scenarios were proposed to explain their particular physical properties (e.g., compact size, low gas content, short depletion time). In this work, we aim at studying the star formation history (SFH) of the GOODS-ALMA galaxies to understand if the so-called ``starburst (SB) in the MS'' galaxies exhibit a different star formation activity over the last Gyr compared to MS galaxies that could explain their specificity. We use the CIGALE SED modelling code to which we add non-parametric SFHs. To compare quantitatively the recent SFH of the galaxies, we define a parameter, the star formation rate (SFR) gradient that provides the angle showing the direction that a galaxy has followed in the SFR vs stellar mass plane over a given period. We show that ``SB in the MS'' have positive or weak negative gradients over the last 100, 300, and 1000 Myr, at odds with a scenario where these galaxies would be transitioning from the SB region at the end of a strong starburst phase. Normal GOODS-ALMA galaxies and ``SB in the MS'' have the same SFR gradients distributions meaning that they have similar recent SFH, despite their different properties (compactness, low depletion time). The ``SBs in the MS'' manage to maintain a star-formation activity allowing them to stay within the MS. This points toward a diversity of galaxies within a complex MS., Comment: Submitted to A&A
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- 2023
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5. Euclid preparation:XXVI. the Euclid Morphology Challenge: Towards structural parameters for billions of galaxies
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Euclid Collaboration, Bretonnière, H., Kuchner, U., Huertas-Company, M., Merlin, E., Castellano, M., Tuccillo, D., Buitrago, F., Conselice, C. J., Boucaud, A., Häußler, B., Kümmel, M., Hartley, W. G., Ayllon, A. Alvarez, Bertin, E., Ferrari, F., Ferreira, L., Gavazzi, R., Hernández-Lang, D., Lucatelli, G., Robotham, A. S. G., Schefer, M., Wang, L., Cabanac, R., Sánchez, H. Domínguez, Duc, P. -A., Fotopoulou, S., Kruk, S., La Marca, A., Margalef-Bentabol, B., Marleau, F. R., Tortora, C., Aghanim, N., Amara, A., Auricchio, N., Azzollini, R., Baldi, M., Bender, R., Bodendorf, C., Branchini, E., Brescia, M., Brinchmann, J., Camera, S., Capobianco, V., Carbone, C., Carretero, J., Castander, F. J., Cavuoti, S., Cimatti, A., Cledassou, R., Congedo, G., Conversi, L., Copin, Y., Corcione, L., Courbin, F., Cropper, M., Da Silva, A., Degaudenzi, H., Dinis, J., Dubath, F., Duncan, C. A. J., Dupac, X., Dusini, S., Farrens, S., Ferriol, S., Frailis, M., Franceschi, E., Fumana, M., Galeotta, S., Garilli, B., Gillis, B., Giocoli, C., Grazian, A., Grupp, F., Haugan, S. V. H., Hoekstra, H., Holmes, W., Hormuth, F., Hornstrup, A., Hudelot, P., Jahnke, K., Kermiche, S., Kiessling, A., Kohley, R., Kunz, M., Kurki-Suonio, H., Ligori, S., Lilje, P. B., Lloro, I., Mansutti, O., Marggraf, O., Markovic, K., Marulli, F., Massey, R., McCracken, H. J., Medinaceli, E., Melchior, M., Meneghetti, M., Meylan, G., Moresco, M., Moscardini, L., Munari, E., Niemi, S. M., Padilla, C., Paltani, S., Pasian, F., Pedersen, K., Percival, W., Pettorino, V., Polenta, G., Poncet, M., Pozzetti, L., Raison, F., Rebolo, R., Renzi, A., Rhodes, J., Riccio, G., Romelli, E., Rosset, C., Rossetti, E., Saglia, R., Sapone, D., Sartoris, B., Schneider, P., Secroun, A., Seidel, G., Sirignano, C., Sirri, G., Skottfelt, J., Starck, J. -L., Tallada-Crespí, P., Taylor, A. N., Tereno, I., Toledo-Moreo, R., Tutusaus, I., Valentijn, E. A., Valenziano, L., Vassallo, T., Wang, Y., Weller, J., Zamorani, G., Zoubian, J., Andreon, S., Bardelli, S., Colodro-Conde, C., Di Ferdinando, D., Graciá-Carpio, J., Lindholm, V., Mauri, N., Mei, S., Scottez, V., Zucca, E., Baccigalupi, C., Ballardini, M., Bernardeau, F., Biviano, A., Borgani, S., Borlaff, A. S., Burigana, C., Cappi, A., Carvalho, C. S., Casas, S., Castignani, G., Cooray, A. R., Coupon, J., Courtois, H. M., Davini, S., De Lucia, G., Desprez, G., Escartin, J. A., Escoffier, S., Fabricius, M., Farina, M., Fontana, A., Ganga, K., Garcia-Bellido, J., George, K., Gozaliasl, G., Hildebrandt, H., Hook, I., Ilbert, O., Ilić, S., Joachimi, B., Kansal, V., Keihanen, E., Kirkpatrick, C. C., Loureiro, A., Macias-Perez, J., Magliocchetti, M., Maoli, R., Marcin, S., Martinelli, M., Martinet, N., Maturi, M., Monaco, P., Morgante, G., Nadathur, S., Nucita, A. A., Patrizii, L., Popa, V., Porciani, C., Potter, D., Pourtsidou, A., Pöntinen, M., Reimberg, P., Sánchez, A. G., Sakr, Z., Schirmer, M., Sefusatti, E., Sereno, M., Stadel, J., Teyssier, R., Valiviita, J., van Mierlo, S. E., Veropalumbo, A., Viel, M., Weaver, J. R., Scott, D., Institut d'astrophysique spatiale (IAS), Université Paris-Sud - Paris 11 (UP11)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS)-Centre National d’Études Spatiales [Paris] (CNES), AstroParticule et Cosmologie (APC (UMR_7164)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité), Laboratoire d'Etude du Rayonnement et de la Matière en Astrophysique et Atmosphères = Laboratory for Studies of Radiation and Matter in Astrophysics and Atmospheres (LERMA), École normale supérieure - Paris (ENS-PSL), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)-CY Cergy Paris Université (CY), Institut d'Astrophysique de Paris (IAP), Institut national des sciences de l'Univers (INSU - CNRS)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Laboratoire d'Astrophysique de Marseille (LAM), Aix Marseille Université (AMU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS), Institut de recherche en astrophysique et planétologie (IRAP), Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire Midi-Pyrénées (OMP), Institut de Recherche pour le Développement (IRD)-Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Institut de Recherche pour le Développement (IRD)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Centre National de la Recherche Scientifique (CNRS), Observatoire astronomique de Strasbourg (ObAS), Université de Strasbourg (UNISTRA)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS), Centre National d'Études Spatiales [Toulouse] (CNES), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut de Physique des 2 Infinis de Lyon (IP2I Lyon), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Astrophysique Interprétation Modélisation (AIM (UMR7158 / UMR_E_9005 / UM_112)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique des Particules de Marseille (CPPM), Aix Marseille Université (AMU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Théorique - UMR CNRS 3681 (IPHT), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Joseph Louis LAGRANGE (LAGRANGE), Université Nice Sophia Antipolis (1965 - 2019) (UNS), COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de la Côte d'Azur, COMUE Université Côte d'Azur (2015-2019) (COMUE UCA)-Université Côte d'Azur (UCA)-Université Côte d'Azur (UCA)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), and Euclid
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Galaxies: fundamental parameters ,Cosmology: observations ,Galaxies: evolution ,FOS: Physical sciences ,Astronomy and Astrophysics ,evolution [Galaxies] ,Astrophysics - Astrophysics of Galaxies ,Methods: data analysis ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,fundamental parameters [Galaxies] ,[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det] ,Astrophysics - Instrumentation and Methods for Astrophysics ,[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph] ,observations [Cosmology] ,data analysis [Methods] ,Instrumentation and Methods for Astrophysics (astro-ph.IM) - Abstract
The various Euclid imaging surveys will become a reference for studies of galaxy morphology by delivering imaging over an unprecedented area of 15 000 square degrees with high spatial resolution. In order to understand the capabilities of measuring morphologies from Euclid-detected galaxies and to help implement measurements in the pipeline, we have conducted the Euclid Morphology Challenge, which we present in two papers. While the companion paper by Merlin et al. focuses on the analysis of photometry, this paper assesses the accuracy of the parametric galaxy morphology measurements in imaging predicted from within the Euclid Wide Survey. We evaluate the performance of five state-of-the-art surface-brightness-fitting codes DeepLeGATo, Galapagos-2, Morfometryka, Profit and SourceXtractor++ on a sample of about 1.5 million simulated galaxies resembling reduced observations with the Euclid VIS and NIR instruments. The simulations include analytic S\'ersic profiles with one and two components, as well as more realistic galaxies generated with neural networks. We find that, despite some code-specific differences, all methods tend to achieve reliable structural measurements (10% scatter on ideal S\'ersic simulations) down to an apparent magnitude of about 23 in one component and 21 in two components, which correspond to a signal-to-noise ratio of approximately 1 and 5 respectively. We also show that when tested on non-analytic profiles, the results are typically degraded by a factor of 3, driven by systematics. We conclude that the Euclid official Data Releases will deliver robust structural parameters for at least 400 million galaxies in the Euclid Wide Survey by the end of the mission. We find that a key factor for explaining the different behaviour of the codes at the faint end is the set of adopted priors for the various structural parameters., Comment: Accepted by A&A. 30 pages, 23+6 figures, Euclid pre-launch key paper. Companion paper: Euclid Collaboration XXV: Merlin et al. 2022 Minor corrections after journal review
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- 2023
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6. Galaxy And Mass Assembly (GAMA)
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Simon P Driver, Sabine Bellstedt, Aaron S G Robotham, Ivan K Baldry, Luke J Davies, Jochen Liske, Danail Obreschkow, Edward N Taylor, Angus H Wright, Mehmet Alpaslan, Steven P Bamford, Amanda E Bauer, Joss Bland-Hawthorn, Maciej Bilicki, Matías Bravo, Sarah Brough, Sarah Casura, Michelle E Cluver, Matthew Colless, Christopher J Conselice, Scott M Croom, Jelte de Jong, Franceso D’Eugenio, Roberto De Propris, Burak Dogruel, Michael J Drinkwater, Andrej Dvornik, Daniel J Farrow, Carlos S Frenk, Benjamin Giblin, Alister W Graham, Meiert W Grootes, Madusha L P Gunawardhana, Abdolhosein Hashemizadeh, Boris Häußler, Catherine Heymans, Hendrik Hildebrandt, Benne W Holwerda, Andrew M Hopkins, Tom H Jarrett, D Heath Jones, Lee S Kelvin, Soheil Koushan, Konrad Kuijken, Maritza A Lara-López, Rebecca Lange, Ángel R López-Sánchez, Jon Loveday, Smriti Mahajan, Martin Meyer, Amanda J Moffett, Nicola R Napolitano, Peder Norberg, Matt S Owers, Mario Radovich, Mojtaba Raouf, John A Peacock, Steven Phillipps, Kevin A Pimbblet, Cristina Popescu, Khaled Said, Anne E Sansom, Mark Seibert, Will J Sutherland, Jessica E Thorne, Richard J Tuffs, Ryan Turner, Arjen van der Wel, Eelco van Kampen, Steve M Wilkins, ITA, USA, GBR, FRA, DEU, AUS, BEL, IND, NLD, POL, ZAF, and Kapteyn Astronomical Institute
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VELOCITY DISPERSIONS ,galaxies: Distances and redshift ,F500 ,Astrophysics::Cosmology and Extragalactic Astrophysics ,distances and redshift ,distances and redshift, galaxies ,luminosity function, mass function, cosmological parameters, Astrophysics - Astrophysics of Galaxies, Astrophysics - Cosmology and Nongalactic Astrophysics ,galaxies: Luminosity function, mass function ,fundamental parameters, galaxies ,TARGET SELECTION ,surveys ,LARGE-SCALE STRUCTURE ,galaxies: Fundamental parameters ,galaxies ,Luminosity function, mass function [galaxies] ,STAR-FORMING GALAXIES ,Astrophysics::Solar and Stellar Astrophysics ,fundamental parameters [galaxies] ,distances and redshift [galaxies] ,luminosity function ,cosmological parameters ,Infrarot-Astrophysik - Abteilung Hinton ,PHOTOMETRIC REDSHIFTS ,QC ,Astrophysics::Galaxy Astrophysics ,catalogues ,QB ,luminosity function [galaxies] ,REDSHIFT SURVEY ,METALLICITY RELATION ,galaxies: Luminosity function ,Astronomy and Astrophysics ,Astrophysics - Astrophysics of Galaxies ,Physics and Astronomy ,Space and Planetary Science ,LUMINOSITY FUNCTION ,mass function ,DIGITAL SKY SURVEY ,MILKY-WAY ,Astrophysics::Earth and Planetary Astrophysics ,fundamental parameters ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
In Galaxy And Mass Assembly Data Release 4 (GAMA DR4), we make available our full spectroscopic redshift sample. This includes 248682 galaxy spectra, and, in combination with earlier surveys, results in 330542 redshifts across five sky regions covering ~250deg^2. The redshift density, is the highest available over such a sustained area, has exceptionally high completeness (95 per cent to r_KIDS=19.65mag), and is well suited for the study of galaxy mergers, galaxy groups, and the low redshift (z, Comment: Accepted for publication in MNRAS. GAMA Data Release 4 is available at: http://www.gama-survey.org/dr4/
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- 2022
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7. Investigating the link between inner gravitational potential and star-formation quenching in CALIFA galaxies
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V. Kalinova, D. Colombo, S. F. Sánchez, E. Rosolowsky, K. Kodaira, R. García-Benito, S. E. Meidt, T. A. Davis, A. B. Romeo, S.-Y. Yu, R. González Delgado, E. A. D. Lacerda, Ministerio de Ciencia e Innovación (España), European Commission, and Natural Sciences and Engineering Research Council of Canada
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Galaxies: fundamental parameters ,Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,bulges [galaxies] ,FOS: Physical sciences ,MASS ,SEQUENCE ,DISK ,Galaxies: structure ,kinematics and dynamics [galaxies] ,fundamental parameters [galaxies] ,BLACK-HOLES ,evolution [galaxies] ,SPIRAL STRUCTURE ,Galaxies: bulges ,SPECTROSCOPY ,Galaxies: star formation ,Galaxies: kinematics and dynamics ,Galaxies: evolution ,Astronomy and Astrophysics ,ATLAS(3D) PROJECT ,Astrophysics - Astrophysics of Galaxies ,EVOLUTION ,Physics and Astronomy ,Space and Planetary Science ,GAS ,Astrophysics of Galaxies (astro-ph.GA) ,structure [galaxies] ,star formation [galaxies] ,CLUSTERS ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited., It has been suggested that gravitational potential can have a significant role in suppressing star formation in nearby galaxies. To establish observational constraints on this scenario, we investigated the connection between the dynamics – taking the circular velocity curves (CVCs) as a proxy for the inner gravitational potential – and star formation quenching in 215 non-active galaxies across the Hubble sequence from the Calar Alto Legacy Integral Field Area (CALIFA) survey. Our results show that galaxies with similar CVCs tend to have a certain star-formation quenching pattern. To explore these findings in more details, we constructed kiloparsec(kpc)-resolved relations of the equivalent width of the Hα (WHα) versus the amplitude (Vc) and shape (β = dlnVc/dlnR) of the circular velocity at given radii. We find that the WHα − Vc is a declining relationship, where the retired regions of the galaxies (the ones with WHα values of below 3 Å) tend to have higher Vc. Concurrently, WHα − β is a bimodal relationship, which is characterised by two peaks: concentration of the star forming regions at a positive β (rising CVC) and a second concentration of the retired regions with a negative β (declining CVC). Our results show that both the amplitude of the CVC – driven by the mass of the galaxies – and its shape – which reflects the internal structure of the galaxies – play an important role in the quenching history of a galaxy. © V. Kalinova et al. 2022., DC acknowledges support by the Deutsche Forschungsgemeinschaft, DFG project number SFB956A. SFS acknowledges Conacyt projects CB-285080 and FC-2016-01 -1916, and PAPIIT-DGAPA IN100519. RGB and RGD acknowledge financial support from the State Agency for Research of the Spanish MCIU through the “Center of Excellence Severo Ochoa” award to the Instituto de Astrofísica de Andalucía (SEV-2017-0709), and the projects AYA2016-77846-P and PID2019-109067-GB100. ER acknowledges the support of the Natural Sciences and Engineering Research Council of Canada (NSERC), funding reference number RGPIN-2017-03987. KK acknowledges deep gratitude to MPIfR in Bonn for the Guest Researchership 2013–2021. In this study, we made use of the data of the first legacy survey, the Calar Alto Legacy Integral Field Area (CALIFA) survey, based on observations made at the Centro Astronómico Hispano Alemán (CAHA) at Calar Alto, operated jointly by the Max Planck-Institut für Astronomie and the Instituto de Astrofísica de Andalucía (CSIC). This research made use of the open-source python packages as Astropy (Astropy Collaboration 2018), SciPy (Virtanen et al. 2020), NumPy (Harris et al. 2020), and Matplotlib (Hunter 2007).
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- 2022
8. Systematic errors on optical-SED stellar mass estimates for galaxies across cosmic time and their impact on cosmology
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Ana Paulino-Afonso, Santiago González-Gaitán, Lluís Galbany, Ana Maria Mourão, Charlotte R. Angus, Mathew Smith, Joseph P. Anderson, Joseph D. Lyman, Hanindyo Kuncarayakti, Myriam Rodrigues, Fundação para a Ciência e a Tecnologia (Portugal), Agencia Estatal de Investigación (España), Ministerio de Ciencia, Innovación y Universidades (España), Villum Fonden, European Commission, European Research Council, and Centre National de la Recherche Scientifique (France)
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Galaxies: fundamental parameters ,Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,Cosmological parameters ,Supernovae: general ,FOS: Physical sciences ,DUST ,Astrophysics::Cosmology and Extragalactic Astrophysics ,DEPENDENCE ,STAR-FORMING GALAXIES ,fundamental parameters [galaxies] ,SUPERNOVA HOST GALAXIES ,SIMPLE-MODEL ,Astrophysics::Solar and Stellar Astrophysics ,cosmological parameters ,Astrophysics::Galaxy Astrophysics ,QB ,LEGACY SURVEY ,IA SUPERNOVAE ,METALLICITY RELATION ,Cosmology: observations ,LUMINOSITIES ,Astronomy and Astrophysics ,HUBBLE-SPACE-TELESCOPE ,Astrophysics - Astrophysics of Galaxies ,observations [cosmology] ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,Astrophysics::Earth and Planetary Astrophysics ,general [supernovae] ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
Studying galaxies at different cosmic epochs entails several observational effects that need to be taken into account to compare populations across a large time-span in a consistent manner. We use a sample of 166 nearby galaxies that hosted type Ia supernovae (SNe Ia) and have been observed with the integral field spectrograph MUSE as part of the AMUSING survey. Here, we present a study of the systematic errors and bias on the host stellar mass with increasing redshift, which are generally overlooked in SNe Ia cosmological analyses. We simulate observations at different redshifts (0.1 < z < 2.0) using four photometric bands (griz, similar to the Dark Energy Survey-SN program) to then estimate the host galaxy properties across cosmic time. We find that stellar masses are systematically underestimated as we move towards higher redshifts, due mostly to different rest-frame wavelength coverage, with differences reaching 0.3 dex at z ∼ 1. We used the newly derived corrections as a function of redshift to correct the stellar masses of a known sample of SN Ia hosts and derive cosmological parameters. We show that these corrections have a small impact on the derived cosmological parameters. The most affected is the value of the mass step ΔM, which is reduced by ∼0.004 (6% lower). The dark energy equation of state parameter w changes by Δw∼ 0.006 (0.6% higher) and the value of Ωm increases at most by 0.001 (∼0.3%), all within the derived uncertainties of the model. While the systematic error found in the estimate of the host stellar mass does not significantly affect the derived cosmological parameters, it is an important source of systematic error that needs to be corrected for as we enter a new era of precision cosmology., This work was supported by Fundação para a Ciência e a Tecnologia (FCT) through the research grant UIDB/00099/2020 and the CRISP project PTDC/FIS-AST-31546/2017. L.G. acknowledges financial support from the Spanish Ministry of Science, Innovation and Universities (MICIU) under the 2019 Ramón y Cajal program RYC2019-027683 and from the Spanish MICIU project HOSTFLOWS PID2020-115253GA-I00. CRA was supported by grants from VILLUM FONDEN (project numbers 16599 and 25501). J.D.L. acknowledges support from a UK Research and Innovation Future Leaders Fellowship (MR/T020784/1). Computations were performed at the cluster “Baltasar-Sete-Sóis”, supported by the H2020 ERC Grant “Matter and strong field gravity: New frontiers in Einstein’s theory” grant agreement no. MaGRaTh-646597, and at COIN, the CosmoStatistics Initiative, whose purchase was made possible due to a CNRS MOMENTUM 2018–2020 under the project “Active Learning for large scale sky surveys”. This work was only possible by the use of the following PYTHON packages: NumPy & SciPy (Walt et al. 2011; Jones et al. 2001), Matplotlib (Hunter 2007), and Astropy (Astropy Collaboration et al. 2013).
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- 2022
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9. The dark matter halo masses of elliptical galaxies as a function of observationally robust quantities
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Alessandro Sonnenfeld, Crescenzo Tortora, Henk Hoekstra, Marika Asgari, Maciej Bilicki, Catherine Heymans, Hendrik Hildebrandt, Konrad Kuijken, Nicola R. Napolitano, Nivya Roy, Edwin Valentijn, and Angus H. Wright
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Astrophysics of Galaxies ,Gravitational lensing ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Galaxies ,Astrophysics ,Astrophysics - Astrophysics of Galaxies ,cD ,CD ,Space and Planetary Science ,weak [gravitational lensing] ,Fundamental parameters ,Astrophysics of Galaxies (astro-ph.GA) ,fundamental parameters [galaxies] ,Galaxies: Elliptical and lenticular ,Weak ,Astrophysics::Galaxy Astrophysics ,elliptical and lenticular [galaxies] - Abstract
Context. The assembly history of the stellar component of a massive elliptical galaxy is closely related to that of its dark matter halo. Measuring how the properties of galaxies correlate with their halo mass can help understand their evolution. Aims. We investigate how the dark matter halo mass of elliptical galaxies varies as a function of their properties, using weak gravitational lensing observations. To minimise the chances of biases, we focus on galaxy properties that can be determined robustly: the surface brightness profile and the colour. Methods. We selected 2409 central massive elliptical galaxies from the SDSS spectroscopic sample. We first measured their surface brightness profile and colours by fitting Sersic models to photometric data from the Kilo-Degree Survey (KiDS). We fitted their halo mass distribution as a function of redshift, rest-frame $r-$band luminosity, half-light radius and rest-frame $u-g$ colour, using KiDS weak lensing data and a Bayesian hierarchical approach. For the sake of robustness to assumptions on the large-radii behaviour of the surface brightness, we repeated the analysis replacing total luminosity and half-light radius with the luminosity within a 10~kpc aperture, $L_{r,10}$, and the light-weighted surface brightness slope, $\Gamma_{10}$. Results. We did not detect any correlation between halo mass and either half-light radius or colour, at fixed redshift and luminosity. Conclusions. Our results indicate that the average star formation efficiency of massive elliptical galaxies has little dependence on their final size or colour. This suggests that the origin of the diversity in the size and colour distribution of these objects lies with properties other than halo mass., Comment: In press on Astronomy & Astrophysics. A short summary video is available at https://youtu.be/LlvwQNjLT7k
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- 2022
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10. Nearby galaxies in the LOFAR Two-metre Sky Survey: I. Insights into the non-linearity of the radio-SFR relation
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V. Heesen, M. Staffehl, A. Basu, R. Beck, M. Stein, F. S. Tabatabaei, M. J. Hardcastle, K. T. Chyży, T. W. Shimwell, B. Adebahr, R. Beswick, D. J. Bomans, A. Botteon, E. Brinks, M. Brüggen, R.-J. Dettmar, A. Drabent, F. de Gasperin, G. Gürkan, G. H. Heald, C. Horellou, B. Nikiel-Wroczynski, R. Paladino, J. Piotrowska, H. J. A. Röttgering, D. J. B. Smith, and C. Tasse
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cosmic rays ,magnetic fields [galaxies] ,Space and Planetary Science ,Galaxies: Halos ,fundamental parameters [galaxies] ,Astronomy and Astrophysics ,Galaxies: Magnetic Fields ,Galaxies: Fundamental Parameters ,Radio Continuum: Galaxies ,Astrophysics - Astrophysics of Galaxies ,galaxies [radio continuum] ,Cosmic Rays ,halos [galaxies] - Abstract
Context. Cosmic rays and magnetic fields are key ingredients in galaxy evolution, regulating both stellar feedback and star formation. Their properties can be studied with low-frequency radio continuum observations that are free from thermal contamination. Aims. We define a sample of 76 nearby (< 30 Mpc) galaxies with rich ancillary data in the radio continuum and infrared from the CHANG-ES and KINGFISH surveys, which will be observed with the LOFAR Two-metre Sky Survey (LoTSS) at 144 MHz. Methods. We present maps for 45 of them as part of the LoTSS data release 2 (LoTSS-DR2), where we measure integrated flux densities and study integrated and spatially resolved radio spectral indices. We investigate the radio–star formation rate (SFR) relation using SFRs derived from total infrared and Hα + 24-μm emission. Results. The radio–SFR relation at 144 MHz is clearly super-linear with L144 MHz ∝ SFR1.4−1.5. The mean integrated radio spectral index between 144 and ≈1400 MHz is ⟨α⟩= − 0.56 ± 0.14, in agreement with the injection spectral index for cosmic ray electrons (CREs). However, the radio spectral index maps show variation of spectral indices with flatter spectra associated with star-forming regions and steeper spectra in galaxy outskirts and, in particular, in extra-planar regions. We found that galaxies with high SFRs have steeper radio spectra; we find similar correlations with galaxy size, mass, and rotation speed. Conclusions. Galaxies that are larger and more massive are better electron calorimeters, meaning that the CRE lose a higher fraction of their energy within the galaxies. This explains the super-linear radio–SFR relation, with more massive, star-forming galaxies being radio bright. We propose a semi-calorimetric radio–SFR relation that employs the galaxy mass as a proxy for the calorimetric efficiency.
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- 2022
11. Effect of AGN on the morphological properties of their host galaxies in the local Universe
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Tilahun Getachew-Woreta, Mirjana Pović, Josefa Masegosa, Jaime Perea, Zeleke Beyoro-Amado, Isabel Márquez, European Commission, Ministerio de Ciencia e Innovación (España), and Ministry of Science and Technology (Ethiopia)
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Galaxies: fundamental parameters ,active [Galaxies] ,Galaxies: evolution ,FOS: Physical sciences ,Astronomy and Astrophysics ,Galaxies: active ,Galaxies: formation ,evolution [Galaxies] ,Astrophysics - Astrophysics of Galaxies ,formation [Galaxies] ,Space and Planetary Science ,nuclei [Galaxies] ,Astrophysics of Galaxies (astro-ph.GA) ,fundamental parameters [Galaxies] ,Galaxies: nuclei - Abstract
The morphological classification of active galaxies may be affected by the presence of active galactic nuclei (AGNs). In this paper, we provide the most detailed analysis on how different AGN contributions, from 5 per cent to 75 per cent, to the total optical light may affect six commonly used morphological parameters and the final classification of AGN host galaxies at z ∼ 0. We used a local sample of > 2000 visually classified non-active galaxies, to quantify how the contribution of a bright nuclear point source of different intensity could affect morphological parameters such as: asymmetry, Abraham concentration index, Gini, M20 moment of light, smoothness, and Conselice-Bershady concentration index. We found that most of the morphological parameters are affected by AGN contributions above 25 per cent, with late-type galaxies being more affected than early-types. We found that Gini, Abraham concentration index, and asymmetry are the most stable parameters even for AGN contributions above 25 per cent, in comparison to Conselice-Bershady concentration index and M20 moment of light. Smoothness parameter shall be avoided when classifying AGN host galaxies, or at least it shall be used simultaneously in combination with several other parameters. © 2022 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society., TGW acknowledges the support from Bule Hora University under the Ministry of Science and Higher Education. TGW, MP, and ZBA acknowledge financial support from the Ethiopian Space Science and Technology Institute (ESSTI) under the Ethiopian Ministry of Innovation and Technology (MInT). TGW, JM, and MP acknowledge support given through the grant CSIC I-COOP 2017 and COOPA20168. MP, JM, JP, and IMP acknowledge the support from the Spanish Ministerio de Ciencia e Innovación - Agencia Estatal de Investigación through projects PID2019-106027GB-C41 and AYA2016-76682C3-1-P, and the State Agency for Research of the Spanish MCIU through the Center of Excellence Severo Ochoa award to the Instituto de Astrofísica de Andalucía (SEV-2017-0709). In this work, we made use of Virtual Observatory Tool for OPerations on Catalogues And Tables (TOPCAT).
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- 2022
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12. Observed structural parameters of EAGLE galaxies: reconciling the mass-size relation in simulations with local observations
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Anna de Graaff, James Trayford, Marijn Franx, Matthieu Schaller, Joop Schaye, and Arjen van der Wel
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Fundamental Parameters ,Evolution ,DATA RELEASE ,DISC GALAXIES ,FOS: Physical sciences ,Astrophysics::Cosmology and Extragalactic Astrophysics ,STAR-FORMATION ,Stellar Content ,fundamental parameters [galaxies] ,ILLUSTRIS SIMULATION ,evolution [galaxies] ,Astrophysics::Galaxy Astrophysics ,Structure ,Astronomy and Astrophysics ,stellar content [galaxies] ,TRANSFER CODE ,Galaxies ,Astrophysics - Astrophysics of Galaxies ,EVOLUTION ,Physics and Astronomy ,DUST RADIATIVE-TRANSFER ,STELLAR POPULATION SYNTHESIS ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,structure [galaxies] ,DIGITAL SKY SURVEY ,MORPHOLOGY - Abstract
We use mock images of $z=0.1$ galaxies in the 100 Mpc EAGLE simulation to establish the differences between the sizes and morphologies inferred from the stellar mass distributions and the optical light distributions. The optical, $r$-band images used were constructed with a radiative transfer method to account for the effects of dust, and we measure galaxy structural parameters by fitting S\'ersic models to the images with Galfit. We find that the derived $r$-band half-light radii differ systematically from the stellar half-mass radii, as the $r$-band sizes are typically 0.1 dex larger, and can deviate by as much as $\approx0.5$ dex. The magnitude of this size discrepancy depends strongly on the dust attenuation and star formation activity within the galaxy, as well as the measurement method used. Consequently, we demonstrate that the $r$-band sizes significantly improve the agreement between the simulated and observed stellar mass-size relation: star-forming and quiescent galaxies in EAGLE are typically only slightly larger than observed in the GAMA survey (by 0.1 dex), and the slope and scatter of the local mass-size relation are reproduced well for both populations. Finally, we also compare the obtained morphologies with measurements from GAMA, finding that too few EAGLE galaxies have light profiles that are similar to local early-type galaxies (S\'ersic indices of $n\sim 4$). Despite the presence of a significant population of triaxial systems among the simulated galaxies, the surface brightness and stellar mass density profiles tend to be closer to exponential discs ($n\sim1-2$). Our results highlight the need to measure the sizes and morphologies of simulated galaxies using common observational methods in order to perform a meaningful comparison with observations., Comment: 22 pages, 18 figures; accepted for publication in MNRAS. The Sersic model parameters are available through the public EAGLE database (see http://icc.dur.ac.uk/Eagle/database.php )
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- 2022
13. [Untitled]
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luminosity function, mass function, cosmological parameters, Astrophysics - Astrophysics of Galaxies, Astrophysics - Cosmology and Nongalactic Astrophysics ,fundamental parameters, galaxies ,surveys ,galaxies ,catalogues ,distances and redshift, galaxies - Published
- 2022
14. GOODS-ALMA 2.0:Starbursts in the main sequence reveal compact star formation regulating galaxy evolution prequenching
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C. Gómez-Guijarro, D. Elbaz, M. Xiao, V. I. Kokorev, G. E. Magdis, B. Magnelli, E. Daddi, F. Valentino, M. T. Sargent, M. Dickinson, M. Béthermin, M. Franco, A. Pope, B. S. Kalita, L. Ciesla, R. Demarco, H. Inami, W. Rujopakarn, X. Shu, T. Wang, L. Zhou, D. M. Alexander, F. Bournaud, R. Chary, H. C. Ferguson, S. L. Finkelstein, M. Giavalisco, D. Iono, S. Juneau, J. S. Kartaltepe, G. Lagache, E. Le Floc’h, R. Leiton, L. Leroy, L. Lin, K. Motohara, J. Mullaney, K. Okumura, M. Pannella, C. Papovich, E. Treister, Astrophysique Interprétation Modélisation (AIM (UMR_7158 / UMR_E_9005 / UM_112)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité), University of Copenhagen = Københavns Universitet (UCPH), Danmarks Tekniske Universitet = Technical University of Denmark (DTU), University of Sussex, Community Science and Data Center, Laboratoire d'Astrophysique de Marseille (LAM), Aix Marseille Université (AMU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS), University of Hertfordshire [Hatfield] (UH), University of Massachusetts [Amherst] (UMass Amherst), University of Massachusetts System (UMASS), Universidad de Concepción - University of Concepcion [Chile], Hiroshima University, Chulalongkorn University [Bangkok], Anhui Normal University, Nanjing University (NJU), Durham University, California Institute of Technology (CALTECH), Space Telescope Science Institute (STSci), University of Texas at Austin [Austin], National Astronomical Observatory of Japan (NAOJ), Rochester Institute of Technology, Academia Sinica, The University of Tokyo (UTokyo), University of Sheffield [Sheffield], Università degli studi di Trieste = University of Trieste, Texas A&M University [College Station], and Pontificia Universidad Católica de Chile (UC)
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submillimeter: galaxies ,SPECTROSCOPIC SURVEY ,Cosmology and Nongalactic Astrophysics (astro-ph.CO) ,SIMILAR-TO 3 ,MASS-METALLICITY RELATION ,INFRARED-EMISSION ,structure [Galaxies] ,FOS: Physical sciences ,Astrophysics::Cosmology and Extragalactic Astrophysics ,star formation [Galaxies] ,star formation ,high-redshift ,high-redshift [Galaxies] ,galaxies [Submillimeter] ,galaxies: high-redshift ,galaxies ,evolution ,DUST TEMPERATURES ,Astrophysics::Solar and Stellar Astrophysics ,submillimeter ,structure ,Astrophysics::Galaxy Astrophysics ,FORMING GALAXIES ,SUBMILLIMETER GALAXIES ,galaxies: fundamental parameters ,Astronomy and Astrophysics ,evolution [Galaxies] ,Astrophysics - Astrophysics of Galaxies ,ORIGINS DEEP SURVEY ,MOLECULAR GAS FRACTIONS ,Space and Planetary Science ,galaxies: star formation ,Astrophysics of Galaxies (astro-ph.GA) ,fundamental parameters [Galaxies] ,galaxies: structure ,Astrophysics::Earth and Planetary Astrophysics ,galaxies: evolution ,[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph] ,fundamental parameters ,Astrophysics - Cosmology and Nongalactic Astrophysics - Abstract
Compact star formation appears to be generally common in dusty star-forming galaxies (SFGs). However, its role in the framework set by the scaling relations in galaxy evolution remains to be understood. In this work we follow up on the galaxy sample from the GOODS-ALMA 2.0 survey, an ALMA blind survey at 1.1mm covering a continuous area of 72.42arcmin$^2$ using two array configurations. We derived physical properties, such as star formation rates, gas fractions, depletion timescales, and dust temperatures for the galaxy sample built from the survey. There exists a subset of galaxies that exhibit starburst-like short depletion timescales, but they are located within the scatter of the so-called main sequence of SFGs. These are dubbed starbursts in the main sequence and display the most compact star formation and they are characterized by the shortest depletion timescales, lowest gas fractions, and highest dust temperatures of the galaxy sample, compared to typical SFGs at the same stellar mass and redshift. They are also very massive, accounting for $\sim 60\%$ of the most massive galaxies in the sample ($\log (M_{\rm{*}}/M_{\odot}) > 11.0$). We find trends between the areas of the ongoing star formation regions and the derived physical properties for the sample, unveiling the role of compact star formation as a physical driver of these properties. Starbursts in the main sequence appear to be the extreme cases of these trends. We discuss possible scenarios of galaxy evolution to explain the results drawn from our galaxy sample. Our findings suggest that the star formation rate is sustained in SFGs by gas and star formation compression, keeping them within the main sequence even when their gas fractions are low and they are presumably on the way to quiescence., Accepted by A&A. 26 pages, 13 figures
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- 2022
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15. Overestimated inclinations of Milgromian disc galaxies: the case of the ultradiffuse galaxy AGC 114905
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Indranil Banik, Srikanth T Nagesh, Hosein Haghi, Pavel Kroupa, Hongsheng Zhao, and University of St Andrews. School of Physics and Astronomy
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MCC ,kinematics and dynamics [Galaxies] ,FOS: Physical sciences ,Astronomy and Astrophysics ,3rd-DAS ,Astrophysics::Cosmology and Extragalactic Astrophysics ,disc [Galaxies] ,individual: AGC 114905 [Galaxies] ,Astrophysics - Astrophysics of Galaxies ,dwarf [Galaxies] ,QC Physics ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,fundamental parameters [Galaxies] ,QB Astronomy ,QC ,Astrophysics::Galaxy Astrophysics ,Gravitation ,QB - Abstract
We present hydrodynamical star-forming simulations in the Milgromian dynamics (MOND) framework of a gas-rich disc galaxy with properties similar to AGC 114905, which has recently been argued to have a rotation curve (RC) that is inconsistent with the MOND prediction. Our first model considers the galaxy in isolation, while our second model includes an external field of $0.05 \, a_{_0}$, the estimated gravitational field from large-scale structure. We show that isophotes in the face-on view can differ from circular at the 50% level. This could mislead observers into overestimating the inclination $i$ between disc and sky planes. Because RCs require a correction factor of $1/\sin i$, the actual RC could be much higher than reported by observers. This plausibly reconciles AGC 114905 with MOND expectations., Comment: 8 pages, 2 figures, 2 tables. Published in the Monthly Notices of the Royal Astronomical Society in this form. Face-on videos available at https://youtu.be/VkZq2Se0_lU (isolated) and https://youtu.be/3wC3yRkrXnc (including an external field of a_0/20)
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- 2022
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16. COSMOS2020: Manifold learning to estimate physical parameters in large galaxy surveys
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Davidzon, I., Jegatheesan, K., Ilbert, O., de la Torre, S., Leslie, S.K., Laigle, C., Hemmati, S., Masters, D.C., Blanquez-Sese, D., Kauffmann, O.B., Magdis, G.E., Małek, K., McCracken, H.J., Mobasher, B., Moneti, A., Sanders, D.B., Shuntov, M., Toft, S., Weaver, J.R., Laboratoire d'Astrophysique de Marseille (LAM), Aix Marseille Université (AMU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS), Institut d'Astrophysique de Paris (IAP), and Institut national des sciences de l'Univers (INSU - CNRS)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)
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H-ALPHA ,FOS: Physical sciences ,SPECTRAL ENERGY-DISTRIBUTIONS ,Astrophysics::Cosmology and Extragalactic Astrophysics ,astronomical databases: miscellaneous ,STAR-FORMATION RATES ,stellar content ,star formation [Galaxies] ,star formation ,methods ,galaxies ,astronomical databases ,observational [Methods] ,observational ,[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det] ,NEAR-INFRARED SURVEY ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,PHOTOMETRIC REDSHIFTS ,Astrophysics::Galaxy Astrophysics ,FORMING GALAXIES ,COMPLETE CALIBRATION ,MASSIVE GALAXIES ,galaxies: fundamental parameters ,Astronomy and Astrophysics ,GALACTIC STELLAR ,Astrophysics - Astrophysics of Galaxies ,miscellaneous ,STELLAR POPULATION SYNTHESIS ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,galaxies: star formation ,fundamental parameters [Galaxies] ,miscellaneous [Astronomical databases] ,galaxies: stellar content ,stellar content [Galaxies] ,methods: observational ,Astrophysics - Instrumentation and Methods for Astrophysics ,[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph] ,fundamental parameters - Abstract
We present a novel method to estimate galaxy physical properties from spectral energy distributions (SEDs), alternate to template fitting techniques and based on self-organizing maps (SOM) to learn the high-dimensional manifold of a photometric galaxy catalog. The method has been previously tested with hydrodynamical simulations in Davidzon et al. (2019) while here is applied to real data for the first time. It is crucial for its implementation to build the SOM with a high quality, panchromatic data set, which we elect to be the "COSMOS2020" galaxy catalog. After the training and calibration steps with COSMOS2020, other galaxies can be processed through SOM to obtain an estimate of their stellar mass and star formation rate (SFR). Both quantities result to be in good agreement with independent measurements derived from more extended photometric baseline, and also their combination (i.e., the SFR vs. stellar mass diagram) shows a main sequence of star forming galaxies consistent with previous studies. We discuss the advantages of this method compared to traditional SED fitting, highlighting the impact of having, instead of the usual synthetic templates, a collection of empirical SEDs built by the SOM in a "data-driven" way. Such an approach also allows, even for extremely large data sets, an efficient visual inspection to identify photometric errors or peculiar galaxy types. Considering in addition the computational speed of this new estimator, we argue that it will play a valuable role in the analysis of oncoming large-area surveys like Euclid or the Legacy Survey of Space and Time at the Vera Cooper Rubin Telescope., Comment: to appear on A&A
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- 2022
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17. Nearby galaxies in the LOFAR Two-metre Sky Survey: III. Influence of cosmic-ray transport on the radio-SFR relation.
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Heesen, V., Schulz, S., Brüggen, M., Edler, H. W., Stein, M., Paladino, R., Boselli, A., Ignesti, A., Fossati, M., and Dettmar, R.-J.
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ASTRONOMICAL surveys ,GALACTIC evolution ,GALAXIES ,GALACTIC magnetic fields ,STAR formation - Abstract
Context. To understand galaxy evolution, it is essential to measure star formation rates (SFRs) across cosmic time. Aims. The use of radio continuum emission as an extinction-free tracer of star formation necessitates a good understanding of the influence of cosmic-ray electron (CRE) transport. Our aim in this work is to improve this understanding. Methods. We analysed the spatially resolved radio continuum-star formation rate (radio-SFR) relation in 15 nearby galaxies using data from the LOw Frequency ARray (LOFAR) and the Westerbork Synthesis Radio Telescope (WSRT) at 144 and 1365 MHz, respectively. The hybrid SFR maps are based on observations with Spitzer at 24 μm and with GALEX at 156 nm. Our pixel-by-pixel analysis at 1.2 kpc resolution reveals the usual sublinear radio-SFR relation for local measurements. This can be linearised with a smoothing experiment, convolving the hybrid SFR map with a Gaussian kernel that provides us with the CRE transport length. Results. CRE transport can be described as energy-independent isotropic diffusion. If we consider only young CREs as identified with the radio spectral index, we find a linear relation showing the influence of cosmic-ray transport. We then define the CRE calorimetric efficiency as the ratio of radio-to-hybrid SFR surface density and show that it is a function of the radio spectral index. If we correct the radio-SFR relation for the CRE calorimetric efficiency parametrised by the radio spectral index, it becomes nearly linear with a slope of 1.01 ± 0.02, independent of frequency. Conclusions. The corrected radio-SFR relation is universal and it holds for both global and local measurements. [ABSTRACT FROM AUTHOR]
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- 2024
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18. Strong size evolution of disc galaxies since z = 1: Readdressing galaxy growth using a physically motivated size indicator.
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Buitrago, Fernando and Trujillo, Ignacio
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DISK galaxies ,GALACTIC evolution ,STELLAR density (Stellar population) ,GALAXIES ,DENSITY of stars - Abstract
Our understanding of how the size of galaxies has evolved over cosmic time is based on the use of the half-light (effective) radius as a size indicator. Although the half-light radius has many advantages for structurally parameterising galaxies, it does not provide a measure of the global extent of the objects, but only an indication of the size of the region containing the innermost 50% of the galaxy's light. Therefore, the observed mild evolution of the effective radius of disc galaxies with cosmic time is conditioned by the evolution of the central part of the galaxies rather than by the evolutionary properties of the whole structure. Expanding on recent works, we studied the size evolution of disc galaxies using the radial location of the gas density threshold for star formation as a size indicator. As a proxy to evaluate this quantity, we used the radial position of the truncation (edge) in the stellar surface mass density profiles of galaxies. To conduct this task, we selected 1048 disc galaxies with M
stellar > 1010 M⊙ and spectroscopic redshifts up to z = 1 within the HST CANDELS fields. We derived their surface brightness, colour and stellar mass density profiles. Using the new size indicator, the observed scatter of the size–mass relation (∼0.1 dex) decreases by a factor of ∼2 compared to that using the effective radius. At a fixed stellar mass, Milky Way-like (MW-like; Mstellar ∼ 5 × 1010 M⊙ ) disc galaxies have, on average, increased their sizes by a factor of two in the last 8 Gyr, while the surface stellar mass density at the edge position (Σedge ) has decreased by more than an order of magnitude from ∼13 M⊙ pc−2 (z = 1) to ∼1 M⊙ pc−2 (z = 0). These results reflect a dramatic evolution of the outer part of MW-like disc galaxies, with an average radial growth rate of its discs of about 1.5 kpc Gyr−1 . [ABSTRACT FROM AUTHOR]- Published
- 2024
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19. Relations between SMBH Parameters and Jet Generation and Efficiency in Blazars.
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Zhang, H. and Zhang, H. J.
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- 2023
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20. Intrinsic dust and star-formation scaling relations in nearby galaxies.
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Pastrav, Bogdan A.
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STAR formation ,PHOTOMETRIC stereo ,STELLAR mass ,GALACTIC evolution - Abstract
Following from our recent work, we present results of a detailed analysis of a representative sample of nearby galaxies. The photometric parameters of the morphological components are obtained from bulge-disk decompositions, using GALFIT software. The previously obtained method and library of numerical corrections for dust, decomposition and projection effects, are used to correct the measured (observed) parameters to intrinsic values. Observed and intrinsic galaxy dust and star-formation related scaling relations are presented, to emphasize the scale of the biases introduced by these effects. To understand the extent to which star-formation is distributed in the young stellar disks of galaxies, star-formation connected relations which rely on measurements of scale-lengths and fluxes/luminosities of Hα images, are shown. The mean dust opacity, dust-to-stellar mass and dust-to-gas ratios of the sample, together with the main characteristics of the intrinsic relations are found to be consistent with values found in the literature. [ABSTRACT FROM AUTHOR]
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- 2023
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21. Lyman continuum leaker candidates among highly ionised, low-redshift dwarf galaxies selected from He ii.
- Author
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Enders, A. U., Bomans, D. J., and Wittje, A.
- Subjects
INTERSTELLAR medium ,ACTIVE galactic nuclei ,DWARF galaxies - Abstract
Context. Contemporary research suggests that the reionisation of the intergalactic medium (IGM) in the early Universe was predominantly realised by star-forming (proto-)galaxies (SFGs). Due to observational constraints, our knowledge on the origins of suffcient amounts of ionising Lyman continuum (LyC) photons and the mechanisms facilitating their transport into the IGM remains sparse. Recent efforts have thus focussed on the study of local analogues to these high-redshift objects. Aims. We aim to acquire a set of very low-redshift SFGs that exhibit signs of a hard radiation field being present. A subsequent analysis of their emission line properties is intended to shed light on how the conditions prevalent in these objects compare to those predicted to be present in early SFGs that are thought to be LyC emitters (LCEs). Methods. We used archival spectroscopic SDSS DR12 data to select a sample of low-redshift He ii 4686 emitters and restricted it to a set of SFGs with an emission line diagnostic sensitive to the presence of an active galactic nucleus, which serves as our only selection criterion. We performed a population spectral synthesis with fado to reconstruct these galaxies' star-formation histories (SFHs). Utilising the spectroscopic information at hand, we constrained the predominant ionisation mechanisms in these galaxies and inferred information on interstellar medium (ISM) conditions relevant for the escape of LyC radiation. Results. Our final sample consists of eighteen ionised, metal-poor galaxies (IMPs). These low-mass (6:2 log (M=M) 8:8), low-metallicity (7:54 log (O=H) + 12 8:13) dwarf galaxies appear to be predominantly ionised by stellar sources. We find large [O iii] 5007/[O ii] 3727 ratios and [S ii] 6717,6731/Hff deficiencies, which provide strong indications for these galaxies to be LCEs. At least 40% of these objects are candidates for featuring cosmologically significant LyC escape fractions &10%. The IMPs' SFHs exhibit strong similarities and almost all galaxies appear to contain an old (>1 Gyr) stellar component, while also harbouring a young, two-stage (~10 Myr and <1 Myr) starburst, which we speculate might be related to LyC escape. Conclusions. The properties of the compact emission line galaxies presented here align well with those observed in many local LCEs. In fact, our sample may prove as an extension to the rather small catalogue of local LCEs, as the extreme ISM conditions we find are assumed to facilitate LyC leakage. Notably, all of our eighteen candidates are significantly closer (z < 0:1) than most established LCEs. If the inferred LyC photon loss is genuine, this demonstrates that selecting SFGs from He ii 4686 is a powerful selection criterion in the search for LCEs. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
22. Diffusion of cosmic-ray electrons in M 51 observed with LOFAR at 54MHz.
- Author
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Heesen, V., de Gasperin, F., Schulz, S., Basu, A., Beck, R., Brüggen, M., Dettmar, R.-J., Stein, M., Gajović, L., Tabatabaei, F. S., and Reichherzer, P.
- Subjects
ELECTRON diffusion ,DISTRIBUTION of stars ,COSMIC rays ,GALACTIC evolution ,GALACTIC magnetic fields ,STAR formation - Abstract
Context. The details of cosmic-ray transport have a strong impact on galaxy evolution. The peak of the cosmic-ray energy distribution is observable in the radio continuum using the electrons as proxy. Aims. We aim to measure the distance that the cosmic-ray electrons (CREs) are transported during their lifetime in the nearby galaxy M 51 across one order of magnitude in cosmic-ray energy (approximately 1-10 GeV). To this end, we use new ultra-low frequency observations from the LOw Frequency ARay (LOFAR) at 54MHz and ancillary data between 144 and 8350 MHz. Methods. As the CREs originate from supernova remnants, the radio maps are smoothed in comparison to the distribution of the star formation. By convolving the map of the star formation rate (SFR) surface density with a Gaussian kernel, we can linearise the radio-SFR relation. The best-fitting convolution kernel is then our estimate of the CRE transport length. Results. We find that the CRE transport length increases at low frequencies, as expected since the CRE have longer lifetimes. The CRE transport length is lCRE = p 4Dtsyn, where D is the isotropic diffusion coeffcient and tsyn is the CRE lifetime as given by synchrotron and inverse Compton losses. We find that the data can be well fitted by diffusion, where D = (2:14 ± 0:13) 1028 cm2 s1. With D / E0:001±0:185, the diffusion coeffcient is independent of the CRE energy E in the range considered. Conclusions. Our results suggest that the transport of GeV-cosmic ray electrons in the star-forming discs of galaxies is governed by energy-independent diffusion. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
23. Lyman-α at cosmic noon I: Lyα spectral type selection of z ∼ 2 – 3 Lyman break galaxies with broadband imaging.
- Author
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Foran, Garry, Cooke, Jeff, Reddy, Naveen, Steidel, Charles, and Shapley, Alice
- Published
- 2023
- Full Text
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24. The Hi in Ring Galaxies Survey (Hi-RINGS)—Effects of the bar on the Hi gas in ring galaxies.
- Author
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Murugeshan, C., Džudžar, R., Bagge, R., O'Beirne, T., Wong, O. I., Kilborn, V. A., Cluver, M. E., Lutz, K. A., and Elagali, A.
- Published
- 2023
- Full Text
- View/download PDF
25. Dashing through the cluster: An X-ray to radio view of UGC 10420 undergoing ram-pressure stripping.
- Author
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Mahajan, Smriti, Singh, Kulinder Pal, Tiwari, Juhi, and Raychaudhury, Somak
- Published
- 2023
- Full Text
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26. GOODS-ALMA 2.0: Starbursts in the main sequence reveal compact star formation regulating galaxy evolution prequenching.
- Author
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Gómez-Guijarro, C., Elbaz, D., Xiao, M., Kokorev, V. I., Magdis, G. E., Magnelli, B., Daddi, E., Valentino, F., Sargent, M. T., Dickinson, M., Béthermin, M., Franco, M., Pope, A., Kalita, B. S., Ciesla, L., Demarco, R., Inami, H., Rujopakarn, W., Shu, X., and Wang, T.
- Subjects
GALACTIC evolution ,COMPACT objects (Astronomy) ,STAR formation ,GALAXY formation ,STARBURSTS ,STELLAR mass - Abstract
Compact star formation appears to be generally common in dusty star-forming galaxies (SFGs). However, its role in the framework set by the scaling relations in galaxy evolution remains to be understood. In this work we follow up on the galaxy sample from the GOODS-ALMA 2.0 survey, an ALMA blind survey at 1.1 mm covering a continuous area of 72.42 arcmin
2 using two array configurations. We derived physical properties, such as star formation rates, gas fractions, depletion timescales, and dust temperatures for the galaxy sample built from the survey. There exists a subset of galaxies that exhibit starburst-like short depletion timescales, but they are located within the scatter of the so-called main sequence of SFGs. These are dubbed starbursts in the main sequence and display the most compact star formation and they are characterized by the shortest depletion timescales, lowest gas fractions, and highest dust temperatures of the galaxy sample, compared to typical SFGs at the same stellar mass and redshift. They are also very massive, accounting for ∼60% of the most massive galaxies in the sample (log(M* /M⊙ ) > 11.0). We find trends between the areas of the ongoing star formation regions and the derived physical properties for the sample, unveiling the role of compact star formation as a physical driver of these properties. Starbursts in the main sequence appear to be the extreme cases of these trends. We discuss possible scenarios of galaxy evolution to explain the results drawn from our galaxy sample. Our findings suggest that the star formation rate is sustained in SFGs by gas and star formation compression, keeping them within the main sequence even when their gas fractions are low and they are presumably on the way to quiescence. [ABSTRACT FROM AUTHOR]- Published
- 2022
- Full Text
- View/download PDF
27. Observed versus simulated halo c–Mvir relations.
- Author
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Leier, Dominik, Ferreras, Ignacio, Negri, Andrea, and Saha, Prasenjit
- Subjects
GRAVITATIONAL lenses ,STELLAR mass ,EXPANDING universe ,DARK matter ,GALAXY clusters ,GALACTIC halos ,GALAXY formation - Abstract
The concentration – virial mass relation is a well-defined trend that reflects the formation of structure in an expanding universe. Numerical simulations reveal a marked correlation that depends on the collapse time of dark matter haloes and their subsequent assembly history. However, observational constraints are mostly limited to the massive end via X-ray emission of the hot diffuse gas in clusters. An alternative approach, based on gravitational lensing over galaxy scales, revealed an intriguingly high concentration at Milky Way-sized haloes. This letter focuses on the robustness of these results by adopting a bootstrapping approach that combines stellar and lensing mass profiles. We also apply the identical methodology to simulated haloes from eagle to assess any systematic. We bypass several shortcomings of ensemble type lens reconstruction and conclude that the mismatch between observed and simulated concentration–to–virial–mass relations are robust, and need to be explained either invoking a lensing-related sample selection bias, or a careful investigation of the evolution of concentration with assembly history. For reference, at a halo mass of 10
12 M⊙ , the concentration of observed lenses is c |$_{12}\, \sim 40\ \pm$| 5, whereas simulations give c |$_{12}\, \sim 15\ \pm$| 1. [ABSTRACT FROM AUTHOR]- Published
- 2022
- Full Text
- View/download PDF
28. Tomography of the Ie-Re and L-Sigma Planes.
- Author
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D'Onofrio, Mauro and Chiosi, Cesare
- Subjects
- *
TOMOGRAPHY , *PLANE geometry , *GALAXIES , *STAR formation , *COMPUTER simulation - Abstract
We have analyzed the distribution of early-type galaxies (ETGs) in the effective surface intensity vs. effective radius ( I e − R e ) plane and in the total luminosity vs. central stellar velocity dispersion ( L − σ ) diagram, with the aim of studying the physical variables that allow the transformation of one space-parameter into the other. We find that the classical Faber–Jackson relation L = L 0 σ α , in which the parameters L 0 and α are confined in a small range of possible values, is incompatible with the distribution observed in the I e − R e plane. The two distributions become mutually consistent only if luminosity is not considered a pure proxy of mass but a variable tightly dependent on the past history of mass assembling and star formation and on the present evolutionary state of the stellar content of a galaxy. The solution comes by considering the L = L 0 ′ σ β law proposed by D'Onofrio et al. in 2020, in which both L 0 ′ and β can vary considerably from galaxy to galaxy. We will also show that the data of the Illustris numerical simulation prove the physical foundation of the L = L 0 ′ σ β law and confirm the prediction of the Zone of Exclusion (ZoE) originating from the intersection of the virial law with the L = L 0 ′ σ β relation. The ZoE is the region in the I e − R e and R e − M s diagrams avoided by real galaxies, and the border of which marks the condition of 'full' virial equilibrium with no recent significant merger events and no undergoing star formation. [ABSTRACT FROM AUTHOR]
- Published
- 2022
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29. Milky Way could invalidate the hypothesis of exotic matter and favor a gravitomagnetic solution to explain dark matter
- Author
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Le Corre, Stéphane
- Published
- 2024
- Full Text
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30. Fundamental Plane of Groups and Clusters of Galaxies: Distances and Pecular Velocities of Superclusters of Galaxies on Small Scales
- Author
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Kopylova, F. G. and Kopylov, A. I.
- Published
- 2024
- Full Text
- View/download PDF
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