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arxiv: 2604.26684 · v1 · submitted 2026-04-29 · 🌌 astro-ph.CO

Recognition: unknown

Euclid preparation. Refining input galaxy shape distributions for shear calibration simulations

Euclid Collaboration: H. Jansen (1) , N. Martinet (2) , S. Grandis (1) , H. Hoekstra (3) , S.-S. Li (4 , 5) , T. Schrabback (1) , G. Congedo (6) , B. Csizi (1) , F. Kleinebreil (1) , G. Mankar (1) , N. Zimmermann (1) , B. Altieri (7) , S. Andreon (8) , N. Auricchio (9) , C. Baccigalupi (10 , 11 , 12 , 13) , M. Baldi (14 , 9 , 15) , S. Bardelli (9) , P. Battaglia (9) , A. Biviano (11 , 10) , E. Branchini (16 , 17 , 8) , M. Brescia (18 , 19) , S. Camera (20 , 21 , 22) , V. Capobianco (22) , C. Carbone (23) , V. F. Cardone (24 , 25) , J. Carretero (26 , 27) , S. Casas (28 , 29) , F. J. Castander (30 , 31) , M. Castellano (24) , G. Castignani (9) , S. Cavuoti (19 , 32) , A. Cimatti (33) , C. Colodro-Conde (34) , L. Conversi (35 , 7) , Y. Copin (36) , F. Courbin (37 , 38 , 39) , H. M. Courtois (40) , M. Cropper (41) , H. Degaudenzi (42) , G. De Lucia (11) , H. Dole (43) , F. Dubath (42) , X. Dupac (7) , S. Escoffier (44) , M. Farina (45) , R. Farinelli (9) , S. Farrens (46) , S. 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Wright (130) ((1) Universit\"at Innsbruck , Institut f\"ur Astro- und Teilchenphysik , Technikerstr. 25/8 , 6020 Innsbruck , Austria , (2) Aix-Marseille Universit\'e , CNRS , CNES , LAM , Marseille , France , (3) Leiden Observatory , Leiden University , Einsteinweg 55 , 2333 CC Leiden , The Netherlands , (4) Kavli Institute for Particle Astrophysics \& Cosmology (KIPAC) , Stanford University , Stanford , CA 94305 , USA , (5) SLAC National Accelerator Laboratory , 2575 Sand Hill Road , Menlo Park , CA 94025 , (6) Institute for Astronomy , University of Edinburgh , Royal Observatory , Blackford Hill , Edinburgh EH9 3HJ , UK , (7) ESAC/ESA , Camino Bajo del Castillo , s/n. , Urb. Villafranca del Castillo , 28692 Villanueva de la Ca\~nada , Madrid , Spain , (8) INAF-Osservatorio Astronomico di Brera , Via Brera 28 , 20122 Milano , Italy , (9) INAF-Osservatorio di Astrofisica e Scienza dello Spazio di Bologna , Via Piero Gobetti 93/3 , 40129 Bologna , (10) IFPU , Institute for Fundamental Physics of the Universe , via Beirut 2 , 34151 Trieste , (11) INAF-Osservatorio Astronomico di Trieste , Via G. B. Tiepolo 11 , 34143 Trieste , (12) INFN , Sezione di Trieste , Via Valerio 2 , 34127 Trieste TS , (13) SISSA , International School for Advanced Studies , Via Bonomea 265 , 34136 Trieste TS , (14) Dipartimento di Fisica e Astronomia , Universit\`a di Bologna , Via Gobetti 93/2 , (15) INFN-Sezione di Bologna , Viale Berti Pichat 6/2 , 40127 Bologna , (16) Dipartimento di Fisica , Universit\`a di Genova , Via Dodecaneso 33 , 16146 , Genova , (17) INFN-Sezione di Genova , (18) Department of Physics "E. Pancini" , University Federico II , Via Cinthia 6 , 80126 , Napoli , (19) INAF-Osservatorio Astronomico di Capodimonte , Via Moiariello 16 , 80131 Napoli , (20) Dipartimento di Fisica , Universit\`a degli Studi di Torino , Via P. Giuria 1 , 10125 Torino , (21) INFN-Sezione di Torino , (22) INAF-Osservatorio Astrofisico di Torino , Via Osservatorio 20 , 10025 Pino Torinese (TO) , (23) INAF-IASF Milano , Via Alfonso Corti 12 , 20133 Milano , (24) INAF-Osservatorio Astronomico di Roma , Via Frascati 33 , 00078 Monteporzio Catone , (25) INFN-Sezione di Roma , Piazzale Aldo Moro , 2 - c/o Dipartimento di Fisica , Edificio G. Marconi , 00185 Roma , (26) Centro de Investigaciones Energ\'eticas , Medioambientales y Tecnol\'ogicas (CIEMAT) , Avenida Complutense 40 , 28040 Madrid , (27) Port d'Informaci\'o Cient\'ifica , Campus UAB , C. Albareda s/n , 08193 Bellaterra (Barcelona) , (28) Institute for Theoretical Particle Physics , Cosmology (TTK) , RWTH Aachen University , 52056 Aachen , Germany , (29) Deutsches Zentrum f\"ur Luft- und Raumfahrt e. V. (DLR) , Linder H\"ohe , 51147 K\"oln , (30) Institute of Space Sciences (ICE , CSIC) , Carrer de Can Magrans , s/n , 08193 Barcelona , (31) Institut d'Estudis Espacials de Catalunya (IEEC) , Edifici RDIT , Campus UPC , 08860 Castelldefels , Barcelona , (32) INFN section of Naples , (33) Dipartimento di Fisica e Astronomia "Augusto Righi" - Alma Mater Studiorum Universit\`a di Bologna , (34) Instituto de Astrof\'isica de Canarias , E-38205 La Laguna , Tenerife , (35) European Space Agency/ESRIN , Largo Galileo Galilei 1 , 00044 Frascati , Roma , (36) Universit\'e Claude Bernard Lyon 1 , CNRS/IN2P3 , IP2I Lyon , UMR 5822 , Villeurbanne , F-69100 , (37) Institut de Ci\`encies del Cosmos (ICCUB) , Universitat de Barcelona (IEEC-UB) , Mart\'i i Franqu\`es 1 , 08028 Barcelona , (38) Instituci\'o Catalana de Recerca i Estudis Avan\c{c}ats (ICREA) , Passeig de Llu\'is Companys 23 , 08010 Barcelona , (39) Institut de Ciencies de l'Espai (IEEC-CSIC) , s/n Cerdanyola del Vall\'es , (40) UCB Lyon 1 , IUF , 4 rue Enrico Fermi , 69622 Villeurbanne , (41) Mullard Space Science Laboratory , University College London , Holmbury St Mary , Dorking , Surrey RH5 6NT , (42) Department of Astronomy , University of Geneva , ch. d'Ecogia 16 , 1290 Versoix , Switzerland , (43) Universit\'e Paris-Saclay , Institut d'astrophysique spatiale , 91405 , Orsay , (44) Aix-Marseille Universit\'e , CPPM , (45) INAF-Istituto di Astrofisica e Planetologia Spaziali , via del Fosso del Cavaliere , 100 , 00100 Roma , (46) Universit\'e Paris-Saclay , Universit\'e Paris Cit\'e , CEA , AIM , 91191 , Gif-sur-Yvette , (47) School of Physics , HH Wills Physics Laboratory , University of Bristol , Tyndall Avenue , Bristol , BS8 1TL , (48) University Observatory , LMU Faculty of Physics , Scheinerstr.~1 , 81679 Munich , (49) Max Planck Institute for Extraterrestrial Physics , Giessenbachstr. 1 , 85748 Garching , (50) INAF-Osservatorio Astronomico di Padova , Via dell'Osservatorio 5 , 35122 Padova , (51) Universit\"ats-Sternwarte M\"unchen , Fakult\"at f\"ur Physik , Ludwig-Maximilians-Universit\"at M\"unchen , 81679 M\"unchen , (52) Institute of Theoretical Astrophysics , University of Oslo , P.O. Box 1029 Blindern , 0315 Oslo , Norway , (53) Jet Propulsion Laboratory , California Institute of Technology , 4800 Oak Grove Drive , Pasadena , CA , 91109 , (54) Department of Physics , Lancaster University , Lancaster , LA1 4YB , (55) Felix Hormuth Engineering , Goethestr. 17 , 69181 Leimen , (56) Technical University of Denmark , Elektrovej 327 , 2800 Kgs. Lyngby , Denmark , (57) Cosmic Dawn Center (DAWN) , (58) Max-Planck-Institut f\"ur Astronomie , K\"onigstuhl 17 , 69117 Heidelberg , (59) NASA Goddard Space Flight Center , Greenbelt , MD 20771 , (60) Department of Physics , Astronomy , Gower Street , London WC1E 6BT , (61) Universit\'e de Gen\`eve , D\'epartement de Physique Th\'eorique , Centre for Astroparticle Physics , 24 quai Ernest-Ansermet , CH-1211 Gen\`eve 4 , (62) Department of Physics , P.O. Box 64 , University of Helsinki , 00014 Helsinki , Finland , (63) Helsinki Institute of Physics , Gustaf H\"allstr\"omin katu 2 , (64) Laboratoire d'etude de l'Univers et des phenomenes eXtremes , Observatoire de Paris , Universit\'e PSL , Sorbonne Universit\'e , 92190 Meudon , (65) SKAO , Jodrell Bank , Lower Withington , Macclesfield SK11 9FT , (66) Centre de Calcul de l'IN2P3/CNRS , 21 avenue Pierre de Coubertin 69627 Villeurbanne Cedex , (67) Universit\"at Bonn , Argelander-Institut f\"ur Astronomie , Auf dem H\"ugel 71 , 53121 Bonn , (68) Dipartimento di Fisica e Astronomia "Augusto Righi" - Alma Mater Studiorum Universit\`a di Bologna , via Piero Gobetti 93/2 , (69) Department of Physics , Institute for Computational Cosmology , Durham University , South Road , Durham , DH1 3LE , (70) Institute of Physics , Laboratory of Astrophysics , Ecole Polytechnique F\'ed\'erale de Lausanne (EPFL) , Observatoire de Sauverny , (71) Telespazio UK S.L. for European Space Agency (ESA) , Urbanizacion Villafranca del Castillo , Villanueva de la Ca\~nada , 28692 Madrid , (72) CEA Saclay , DFR/IRFU , Service d'Astrophysique , Bat. 709 , 91191 Gif-sur-Yvette , (73) Institut de F\'isica d'Altes Energies (IFAE) , The Barcelona Institute of Science , Technology , (74) European Space Agency/ESTEC , Keplerlaan 1 , 2201 AZ Noordwijk , (75) School of Mathematics , Statistics , Physics , Newcastle University , Herschel Building , Newcastle-upon-Tyne , NE1 7RU , (76) DARK , Niels Bohr Institute , University of Copenhagen , Jagtvej 155 , 2200 Copenhagen , (77) Waterloo Centre for Astrophysics , University of Waterloo , Waterloo , Ontario N2L 3G1 , Canada , (78) Department of Physics , (79) Perimeter Institute for Theoretical Physics , Ontario N2L 2Y5 , (80) Space Science Data Center , Italian Space Agency , via del Politecnico snc , 00133 Roma , (81) Institute of Space Science , Str. Atomistilor , nr. 409 M\u{a}gurele , Ilfov , 077125 , Romania , (82) Dipartimento di Fisica e Astronomia "G. Galilei" , Universit\`a di Padova , Via Marzolo 8 , 35131 Padova , (83) INFN-Padova , (84) Instituto de F\'isica Te\'orica UAM-CSIC , Campus de Cantoblanco , 28049 Madrid , (85) Institut de Recherche en Astrophysique et Plan\'etologie (IRAP) , Universit\'e de Toulouse , UPS , 14 Av. Edouard Belin , 31400 Toulouse , (86) Universit\'e St Joseph , Faculty of Sciences , Beirut , Lebanon , (87) Departamento de F\'isica , FCFM , Universidad de Chile , Blanco Encalada 2008 , Santiago , Chile , (88) Department of Physics , Helsinki Institute of Physics , (89) Departamento de F\'isica , Faculdade de Ci\^encias , Universidade de Lisboa , Edif\'icio C8 , Campo Grande , PT1749-016 Lisboa , Portugal , (90) Instituto de Astrof\'isica e Ci\^encias do Espa\c{c}o , Tapada da Ajuda , 1349-018 Lisboa , (91) Cosmic Dawn Center (DAWN) , (92) Niels Bohr Institute , Jagtvej 128 , (93) Universidad Polit\'ecnica de Cartagena , Departamento de Electr\'onica y Tecnolog\'ia de Computadoras , Plaza del Hospital 1 , 30202 Cartagena , (94) Kapteyn Astronomical Institute , University of Groningen , PO Box 800 , 9700 AV Groningen , (95) Caltech/IPAC , 1200 E. California Blvd. , CA 91125 , (96) Dipartimento di Fisica e Scienze della Terra , Universit\`a degli Studi di Ferrara , Via Giuseppe Saragat 1 , 44122 Ferrara , (97) Istituto Nazionale di Fisica Nucleare , Sezione di Ferrara , (98) Universit\'e Paris Cit\'e , Astroparticule et Cosmologie , 75013 Paris , (99) INAF , Istituto di Radioastronomia , Via Piero Gobetti 101 , (100) INFN-Bologna , Via Irnerio 46 , 40126 Bologna , (101) Astronomical Observatory of the Autonomous Region of the Aosta Valley (OAVdA) , Loc. Lignan 39 , I-11020 , Nus (Aosta Valley) , (102) Universit\'e C\^ote d'Azur , Observatoire de la C\^ote d'Azur , Laboratoire Lagrange , Bd de l'Observatoire , CS 34229 , 06304 Nice cedex 4 , (103) ICSC - Centro Nazionale di Ricerca in High Performance Computing , Big Data e Quantum Computing , Via Magnanelli 2 , Bologna , (104) Univ. Grenoble Alpes , Grenoble INP , LPSC-IN2P3 , 53 , Avenue des Martyrs , 38000 , Grenoble , (105) Dipartimento di Fisica , Sapienza Universit\`a di Roma , Piazzale Aldo Moro 2 , (106) Aurora Technology for European Space Agency (ESA) , (107) Dipartimento di Fisica - Sezione di Astronomia , Universit\`a di Trieste , Via Tiepolo 11 , 34131 Trieste , (108) Institut d'Astrophysique de Paris , 98bis Boulevard Arago , 75014 , Paris , (109) ICL , Junia , Universit\'e Catholique de Lille , LITL , 59000 Lille , (110) CERCA/ISO , Department of Physics , Case Western Reserve University , 10900 Euclid Avenue , Cleveland , OH 44106 , (111) Laboratoire Univers et Th\'eorie , (112) Dipartimento di Fisica "Aldo Pontremoli" , Universit\`a degli Studi di Milano , Via Celoria 16 , (113) INFN-Sezione di Milano , (114) Departamento de F\'isica Fundamental. Universidad de Salamanca. 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De Giorgi , University of Salento , CP-I93 , (125) INAF-Sezione di Lecce , c/o Dipartimento Matematica e Fisica , (126) Institut d'Astrophysique de Paris , UMR 7095 , 98 bis boulevard Arago , 75014 Paris , (127) Institute of Cosmology , Gravitation , University of Portsmouth , Portsmouth PO1 3FX , (128) Department of Computer Science , Aalto University , PO Box 15400 , Espoo , FI-00 076 , (129) Universidad de La Laguna , Dpto. Astrof\'i sica , E-38206 La Laguna , (130) Ruhr University Bochum , Faculty of Physics , Astronomical Institute (AIRUB) , German Centre for Cosmological Lensing (GCCL) , 44780 Bochum , (131) Department of Physics , Vesilinnantie 5 , University of Turku , 20014 Turku , (132) Finnish Centre for Astronomy with ESO (FINCA) , Quantum , (133) Serco for European Space Agency (ESA) , (134) ARC Centre of Excellence for Dark Matter Particle Physics , Melbourne , Australia , (135) Centre for Astrophysics \& Supercomputing , Swinburne University of Technology , Hawthorn , Victoria 3122 , (136) Department of Physics , University of the Western Cape , Bellville , Cape Town , 7535 , South Africa , (137) Department of Physics , Oxford University , Keble Road , Oxford OX1 3RH , (138) DAMTP , Centre for Mathematical Sciences , Wilberforce Road , Cambridge CB3 0WA , (139) Kavli Institute for Cosmology Cambridge , Madingley Road , Cambridge , CB3 0HA , (140) Departement of Theoretical Physics , (141) Department of Physics , Centre for Extragalactic Astronomy , (142) IRFU , Universit\'e Paris-Saclay 91191 Gif-sur-Yvette Cedex , (143) INAF-Osservatorio Astrofisico di Arcetri , Largo E. Fermi 5 , 50125 , Firenze , (144) Centro de Astrof\'isica da Universidade do Porto , Rua das Estrelas , 4150-762 Porto , (145) Instituto de Astrof\'isica e Ci\^encias do Espa\c{c}o , Universidade do Porto , CAUP , PT4150-762 Porto , (146) HE Space for European Space Agency (ESA) , (147) Department of Astrophysics , University of Zurich , Winterthurerstrasse 190 , 8057 Zurich , (148) University of Applied Sciences , Arts of Northwestern Switzerland , School of Computer Science , 5210 Windisch , (149) INAF - Osservatorio Astronomico d'Abruzzo , Via Maggini , 64100 , Teramo , (150) Theoretical astrophysics , Uppsala University , Box 516 , 751 37 Uppsala , Sweden , (151) Department of Physics , Duke University , Box 90305 , NC 27708 , (152) Mathematical Institute , University of Leiden , 2333 CA Leiden , (153) Institute of Astronomy , University of Cambridge , Cambridge CB3 0HA , (154) Center for Astrophysics , Cosmology , University of Nova Gorica , Nova Gorica , Slovenia , (155) Institute for Particle Physics , Astrophysics , Dept. of Physics , ETH Zurich , Wolfgang-Pauli-Strasse 27 , 8093 Zurich , (156) Department of Astrophysical Sciences , Peyton Hall , Princeton University , Princeton , NJ 08544 , (157) Fakult\"at f\"ur Physik , Universit\"at Bielefeld , Postfach 100131 , 33501 Bielefeld , (158) Space physics , astronomy research unit , University of Oulu , Pentti Kaiteran katu 1 , FI-90014 Oulu , (159) International Centre for Theoretical Physics (ICTP) , Strada Costiera 11 , (160) Center for Computational Astrophysics , Flatiron Institute , 162 5th Avenue , 10010 , New York , NY , USA)

Authors on Pith no claims yet

Pith reviewed 2026-05-07 11:35 UTC · model grok-4.3

classification 🌌 astro-ph.CO
keywords galaxy morphologyweak gravitational lensingshear calibrationEuclid surveySersic profilesimage simulationsmultiplicative biasFlagship mock
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The pith

Updated galaxy morphologies from real Euclid data change the simulated multiplicative shear bias by a percent level, exceeding the mission error budget by a factor of five.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper extracts galaxy shape parameters from deep Euclid observations using single and double-Sersic model fits with SourceXtractor++. It trains a pipeline on this data to augment the morphological distributions in the Flagship mock catalogue and then generates new image simulations for shear calibration. These updated simulations produce a percent-level shift in the multiplicative bias relative to the original Flagship inputs. The shift is five times larger than Euclid's allowed systematic error, showing that morphological accuracy directly limits the precision of weak-lensing cosmology. The work also maps the bias sensitivity to individual morphological parameters and verifies that the refined pipeline meets the requirements for the first data release.

Core claim

Fitting single and double-Sersic profiles to deep-field Euclid images and training a simulation pipeline on the resulting distributions yields image simulations whose multiplicative shear bias differs from the original Flagship morphology at the percent level; this difference exceeds Euclid's tight error budget by a factor of five.

What carries the argument

Single and double-Sersic model fits extracted from deep Euclid fields with SourceXtractor++, used to retrain and replace the morphological distributions supplied to shear-calibration image simulations.

If this is right

  • The percent-level bias change must be absorbed into the shear calibration pipeline before cosmological parameter estimation.
  • Sensitivity of the bias to bulge-to-disk ratio and size parameters requires that these quantities be controlled at the level already achieved by the trained pipeline.
  • The same training approach satisfies the systematic-error allocation for the first data-release cosmology analysis.
  • Double-Sersic models reduce the residual bias relative to single-Sersic models, indicating that two-component structure matters at the required precision.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Similar deep-field training may be needed for other wide-field lensing surveys whose mock catalogues were built with simpler morphological prescriptions.
  • If the deep-to-wide generalization holds, the method can be re-applied to later Euclid data releases with only updated auxiliary fields.
  • A mismatch between simulated and observed morphology distributions could contribute to the scatter seen in shear measurements across different surveys.

Load-bearing premise

Single and double-Sersic fits to the deep-field data accurately represent the morphological distributions that drive shear bias in the full Euclid Wide Survey.

What would settle it

Measuring the multiplicative bias on real Euclid Wide Survey data and checking whether it lies closer to the updated simulation value than to the original Flagship value would directly test the claim.

Figures

Figures reproduced from arXiv: 2604.26684 by 00014 Helsinki, 00044 Frascati, 00078 Monteporzio Catone, 00100 Roma, 00133 Roma, 00185 Roma, 0315 Oslo, 06304 Nice cedex 4, 077125, 08010 Barcelona, 08028 Barcelona, 08193 Barcelona, 08193 Bellaterra (Barcelona), 08860 Castelldefels, 10, 10), 100, 100), 10010, 10025 Pino Torinese (TO), (100) INFN-Bologna, 10125 Torino, (101) Astronomical Observatory of the Autonomous Region of the Aosta Valley (OAVdA), (102) Universit\'e C\^ote d'Azur, 103), (103) ICSC - Centro Nazionale di Ricerca in High Performance Computing, (104) Univ. 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Figure 1
Figure 1. Figure 1: The COSMOS field as observed by Euclid with the correspond￾ing MER tiles at EWS depth. The deep field covers about the same area with smaller tiles. We also show the HEALpix belonging to each tile and the underlying galaxy density in the background. stars in the deeper stacks due to the extended faint light haloes of their images. The stars are masked by MER by scaling a tem￾plate depending on the magnitud… view at source ↗
Figure 3
Figure 3. Figure 3: Difference between joint and individual fitting. We notice that the residuals for a joint fit look like noise, while the individual fitting has clear structure. The fainter galaxy is over-corrected, because flux of the brighter one is being associated with it. ponents ϵ1 = |ϵ| cos(2 α), (7) ϵ2 = |ϵ| sin(2 α), (8) where α denotes the orientation angle of the major axis. We also control the box size in which… view at source ↗
Figure 2
Figure 2. Figure 2: Representative mask for one of the used tiles. We show the stellar masks, as well as the ghost masks, and custom masks for bright objects view at source ↗
Figure 4
Figure 4. Figure 4: Generic example of model fitting on a 150 × 150 pixel cutout. Stars are not fitted for. Both residuals look consistent with noise at the modeled positions indicating that the fitting works well view at source ↗
Figure 5
Figure 5. Figure 5: Simulated stellar densities in the COSMOS field compared to the observed ones and the masked stars. The observed distribution was determined using POINT_LIKE_PROB > 0.8 as a cut for the MER cata￾logue. cut on the MER catalogue. It is evident that both distributions agree very well. The observed distribution does not cover the full magnitude range, because very bright stars are saturated and masked. To illu… view at source ↗
Figure 7
Figure 7. Figure 7: Exposure time variation of one of the used deep MER tiles. One can see a strong gradient in the exposure time towards the upper part of the image, where more VIS observations overlap. noise was introduced due to a bilinear resampling. Additionally, imperfection in the spatially dependent background subtraction can introduce noise correlations on large scales. The MER RMS map accounts for this additional co… view at source ↗
Figure 8
Figure 8. Figure 8: Distribution of exposure times and background values over the field of view of the mosaics. The blue histogram shows the distribu￾tion of exposure times, while the lines show the behaviour of the back￾ground RMS given the exposure time. Dashed lines highlight the fitted behaviour for the RMS. trum and scaled them to the variance needed at a certain expo￾sure time. We found that the RMS, which accounts for … view at source ↗
Figure 10
Figure 10. Figure 10: Comparison between input galaxy parameters and recovered galaxy parameters from the image simulations. The half-light radius rhl in arcsecond is displayed logarithmically here. The upper row shows isolated sources defined as having no neighbour within 1′′. The lower row indicates blended sources as those that have a neighbour within that radius. While most objects follow the identity line, there is also a… view at source ↗
Figure 11
Figure 11. Figure 11: Magnitude distribution of the real data for different exposure time ranges. The solid lines are kernel density estimates of the magni￾tude distribution in a given exposure time bin. As expected the longer we expose the more faint galaxies can be recovered. one magnitude depending on the exposure time. If we simulate a shallow part of the real data, we therefore do not need to include the faintest galaxy p… view at source ↗
Figure 12
Figure 12. Figure 12: Detection probability validation. The left panel shows the be￾havior of the detection probability with magnitude. In the right panel we show the magnitude histogram with the detection probability as weights. exposure time bin. Using the KDE allows us to have a contin￾uous estimate of the density over the whole magnitude range. To calculate the weight factor described by Eq. (18), we inter￾polate between t… view at source ↗
Figure 13
Figure 13. Figure 13: Sensitivity determination for a mean shift in the absolute value of the ellipticity ϵ. We show here the residual bias with respect to a ref￾erence simulation. The measurement bias arises solely from the shear measurement code (LensMC in this case), while the detection bias orig￾inates from a detection preference that correlates with the shear signal. The weight bias accounts for the difference between a w… view at source ↗
Figure 14
Figure 14. Figure 14: Comparison of core parameters between real data and image simulations in normalized histograms. The lower panel of each subplot shows the relative difference between image simulations and real data for each of the histogram bins. The image simulations are either based on the copulae or on the Flagship galaxy mock catalogue directly. 17.0 19.0 21.0 23.0 25.0 27.0 29.0 IE 10−2 10−1 100 101 102 n [arcmin −2 … view at source ↗
Figure 15
Figure 15. Figure 15: Number density of galaxies for the EDL-COSMOS field and the simulations. The left panel shows the histogram, while the right panel shows the ratio between the simulations and the reference data in each magnitude bin. The blue and orange shaded regions depict the 1σ and 2σ margins expected from sample variance. ies in our simulations, we removed galaxies at that magnitude with a 50% probability from the sa… view at source ↗
Figure 16
Figure 16. Figure 16: Half-light radius comparison in arbitrary magnitude bins in comparison to the EDL-COSMOS observations. The upper panels show the augmented and Flagship simulations compared to the EDL-COSMOS data. The lower panels show the relative difference between the histograms and the reference sample. The error bars depict the Poisson uncertainty due to the number of galaxies in each bin. In gray we show the 10% dev… view at source ↗
Figure 17
Figure 17. Figure 17: Ellipticity comparison in arbitrary magnitude bins in comparison to the real data using the EDL-COSMOS observations. The upper panels show the augmented and Flagship simulations compared to the EDL-COSMOS data. The lower panels show the relative difference between the histograms and the reference sample. The error bars depict the Poisson uncertainty due to the number of galaxies in each bin. In gray we sh… view at source ↗
Figure 18
Figure 18. Figure 18: Same as view at source ↗
Figure 19
Figure 19. Figure 19: Same as view at source ↗
Figure 20
Figure 20. Figure 20: Same as view at source ↗
Figure 21
Figure 21. Figure 21: Ellipticity comparison in arbitrary redshift bins in comparison to the real data using the EWL-COSMOS observations. The upper panels show the augmented and Flagship simulations compared to the EWL-COSMOS data. The lower panels show the relative difference between the histograms and the reference sample. The error bars depict the Poisson uncertainty due to the number of galaxies in each bin. In gray we sho… view at source ↗
read the original abstract

The Euclid Wide Survey (EWS) will cover the majority of the extragalactic sky with a resolution similar to the Hubble Space Telescope. This unprecedented data set will introduce a new era of precision cosmology. However, systematic effects need to be controlled better than ever. One of the sources of systematic uncertainties in weak gravitational lensing are biases introduced during the shear measurement. Determining these biases precisely allows the calibration of cosmological measurements to within Euclid's required accuracy. The simulations that are used to determine such biases, need to resemble the real observations. In this work, we aim to learn distributions of galaxy shape parameters from real Euclid data and use the new information to augment the morphological information in the Flagship galaxy mock catalogue. The morphology is extracted using single and double-S\'ersic model fits to the real data, for which we use SourceXtractor++. We train our pipeline on deep Euclid observations of a field with rich auxiliary data and then use it to simulate EWS-like data. In these simulations we compare the multiplicative bias between the morphology from the Flagship catalogue, the trained single-S\'ersic morphology, and the trained double-S\'ersic morphology. We find that the image simulations with the updated morphology result in a percent-level change in the multiplicative shear bias compared to the original morphology from Flagship. This bias exceeds Euclid's tight error budget by a factor of five and underlines the need for this work. Furthermore, we study the sensitivity of the multiplicative bias to key morphological parameters and show that our approach satisfies the requirements for the cosmology analysis with the first data release of Euclid.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The manuscript develops a pipeline to extract single- and double-Sérsic morphological parameters from deep Euclid auxiliary fields using SourceXtractor++, trains distributions on these data, and augments the Flagship mock catalogue. Image simulations are then run with the original Flagship morphologies versus the updated single-Sérsic and double-Sérsic versions; the resulting multiplicative shear bias shifts by a percent-level amount that exceeds Euclid's allocated error budget by a factor of five. The work also examines the sensitivity of this bias to key morphological parameters and concludes that the refined approach satisfies requirements for the first data release cosmology analysis.

Significance. If the central result is robust, the paper is significant for Euclid preparation because it quantifies how input morphology inaccuracies can propagate into shear calibration biases that violate the mission's tight systematic budget, thereby motivating updates to simulation pipelines. The use of real deep-field data to inform mocks and the explicit sensitivity study are strengths that align with the need for reproducible, data-driven calibration.

major comments (2)
  1. [§4] §4 (training and application pipeline): the central claim that the observed percent-level shift in multiplicative bias is attributable to morphology rather than simulation artifacts rests on the assumption that single/double-Sérsic fits to deep fields generalize to EWS depth and selection; no explicit cross-check or bias test at shallower S/N and under the EWS selection function is reported, which is load-bearing for interpreting the factor-of-five excess.
  2. [Results] Results section (bias comparison): the headline finding of a percent-level change exceeding the budget by a factor of five is stated without accompanying error bars, sample statistics, fit-quality metrics, or validation against independent data, as required to assess whether the delta-m is statistically significant and not driven by noise or selection mismatch.
minor comments (1)
  1. [Abstract] Abstract: the statement that the updated morphology 'satisfies the requirements for the cosmology analysis with the first data release' would benefit from a brief quantitative statement of the residual bias level after the update.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their constructive review and positive assessment of the work's significance for Euclid preparation. We address each major comment below, indicating revisions where appropriate to strengthen the manuscript.

read point-by-point responses
  1. Referee: [§4] §4 (training and application pipeline): the central claim that the observed percent-level shift in multiplicative bias is attributable to morphology rather than simulation artifacts rests on the assumption that single/double-Sérsic fits to deep fields generalize to EWS depth and selection; no explicit cross-check or bias test at shallower S/N and under the EWS selection function is reported, which is load-bearing for interpreting the factor-of-five excess.

    Authors: We appreciate the referee drawing attention to the generalization from deep-field training data to EWS conditions. The auxiliary fields were chosen precisely to enable high-S/N morphology fits with SourceXtractor++ that are not feasible at EWS depth; the resulting parameter distributions are then injected into image simulations that explicitly match EWS depth, noise, and selection. Internal checks within the auxiliary data confirm that the fitted distributions remain stable when subsets at moderately lower S/N are used. We acknowledge that a direct end-to-end test fitting morphologies on EWS-depth mocks would further strengthen the interpretation. In the revised manuscript we will add a dedicated paragraph in §4 discussing the S/N dependence of Sérsic recovery, the rationale for deep-field training, and the steps taken to align the simulation selection function with EWS, thereby clarifying that the reported bias shift arises from the updated morphology inputs. revision: partial

  2. Referee: [Results] Results section (bias comparison): the headline finding of a percent-level change exceeding the budget by a factor of five is stated without accompanying error bars, sample statistics, fit-quality metrics, or validation against independent data, as required to assess whether the delta-m is statistically significant and not driven by noise or selection mismatch.

    Authors: We agree that the results section would benefit from explicit statistical characterization. The bias measurements are derived from large simulated samples (approximately 10^6 galaxies per morphology configuration, drawn from the Flagship catalogue after applying the EWS-like selection). In the revised manuscript we will report the statistical uncertainties on each multiplicative bias value, the exact galaxy counts and variance estimates used, reduced-χ² distributions for the single- and double-Sérsic fits, and a direct comparison of the selection function between the original Flagship and the updated catalogues. These additions will allow readers to confirm that the percent-level shift exceeds both the statistical error and the Euclid error budget by the stated factor. revision: yes

Circularity Check

0 steps flagged

No significant circularity: empirical simulation comparison is self-contained

full rationale

The paper extracts Sersic parameters from deep auxiliary Euclid data via SourceXtractor++, augments the Flagship mock, and measures the resulting change in multiplicative shear bias by re-running the same image simulations. This is a direct numerical delta obtained from explicit forward modeling rather than any algebraic derivation or fitted parameter renamed as a prediction. No equations reduce the reported percent-level bias shift to the input fits by construction, and no load-bearing uniqueness theorems or self-citation chains are invoked to justify the central result. The analysis therefore rests on independent simulation outputs and satisfies the criteria for a non-circular finding.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

No free parameters, axioms, or invented entities are introduced; the work relies on standard Sersic profile fitting and the pre-existing Flagship catalogue.

pith-pipeline@v0.9.0 · 12160 in / 1159 out tokens · 38193 ms · 2026-05-07T11:35:23.835330+00:00 · methodology

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Works this paper leans on

2 extracted references · 1 canonical work pages

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