Université de Lausanne
Face recognition models are trained on large-scale datasets, which have privacy and ethical concerns. Lately, the use of synthetic data to complement or replace genuine data for the training of face recognition models has been proposed. While promising results have been obtained, it still remains unclear if generative models can yield diverse enough data for such tasks. In this work, we introduce a new method, inspired by the physical motion of soft particles subjected to stochastic Brownian forces, allowing us to sample identities distributions in a latent space under various constraints. We introduce three complementary algorithms, called Langevin, Dispersion, and DisCo, aimed at generating large synthetic face datasets. With this in hands, we generate several face datasets and benchmark them by training face recognition models, showing that data generated with our method exceeds the performance of previously GAN-based datasets and achieves competitive performance with state-of-the-art diffusion-based synthetic datasets. While diffusion models are shown to memorize training data, we prevent leakage in our new synthetic datasets, paving the way for more responsible synthetic datasets.
Researchers developed a rigorous mathematical framework for characterizing carbon (p,q)-nanotubes by expressing their "random eigenvalues" as functionals of independent uniform distributions. The work provides explicit formulas for probability density functions and moment generating functions for specific nanotube types, establishes their asymptotic convergence to the infinite triangular lattice, and includes a numerical algorithm for analyzing chiral structures.
University of Toronto logoUniversity of TorontoUniversity of Amsterdam logoUniversity of AmsterdamCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of Illinois at Urbana-Champaign logoUniversity of Illinois at Urbana-ChampaignUniversity of OsloUniversity of Cambridge logoUniversity of CambridgeUniversity of ZurichUniversity of Southern California logoUniversity of Southern CaliforniaUniversity of Chicago logoUniversity of ChicagoTel Aviv University logoTel Aviv UniversityUniversity College London logoUniversity College LondonUniversity of Oxford logoUniversity of OxfordUniversity of California, Irvine logoUniversity of California, IrvineUniversity of Copenhagen logoUniversity of CopenhagenUniversity of EdinburghUniversity of British Columbia logoUniversity of British ColumbiaUniversity of CreteKavli Institute for the Physics and Mathematics of the UniverseUniversity of Florida logoUniversity of FloridaINFN Sezione di PisaSpace Telescope Science Institute logoSpace Telescope Science InstituteInstitute for Advanced StudyUniversité Paris-Saclay logoUniversité Paris-SaclayHelsinki Institute of PhysicsStockholm University logoStockholm UniversityUniversity of HelsinkiThe University of ManchesterUniversité de GenèveAalto University logoAalto UniversityQueen Mary University of London logoQueen Mary University of LondonUniversity of PortsmouthMax Planck Institute for AstrophysicsUniversity of IcelandUniversity of NaplesUniversiteit LeidenUniversity of SussexDurham University logoDurham UniversityNiels Bohr InstituteUniversity of JyväskyläUniversity of PadovaInstituto de Astrofísica de CanariasUniversity of the WitwatersrandUniversity of NottinghamEuropean Space AgencyUniversity of Cape TownUniversity of LisbonINFN, Sezione di TorinoPontificia Universidad Católica de ChileDublin Institute for Advanced StudiesJodrell Bank Centre for AstrophysicsINFN, Laboratori Nazionali di FrascatiUniversity of the Basque CountryUniversity of Hawai’iINFN, Sezione di MilanoUniversity of KwaZulu-NatalLudwig-Maximilians-UniversitätInstituto de Astrofísica de Andalucía-CSICUniversity of the Western CapeINAF – Istituto di Astrofisica Spaziale e Fisica Cosmica MilanoLaboratoire d’Astrophysique de MarseilleKavli IPMU (WPI), UTIAS, The University of TokyoMax-Planck Institut für extraterrestrische PhysikINAF-Istituto di RadioastronomiaINAF - Osservatorio di Astrofisica e Scienza dello SpazioLebanese UniversityCambridge UniversityUniversité de MarseilleINFN - Sezione di PadovaINAF-IASF MilanoCosmic Dawn CenterINFN-Sezione di BolognaINFN Sezione di RomaINAF-Osservatorio Astronomico di BolognaINFN Sezione di Roma Tor VergataNational Astronomical Observatories of ChinaSISSA - Scuola Internazionale Superiore di Studi AvanzatiUniversité de LausanneCEA Paris-SaclayUniversity of Oslo, Institute of Theoretical AstrophysicsParis SaclayNational Institute for Physics and Nuclear EngineeringExeter UniversityUniversity of Helsinki, Department of PhysicsUniversité Paris-Saclay, CNRSUniversité de Genève, Département d’AstronomieParis Institute of AstrophysicsAPC, UMR 7164, Université Paris Cité, CNRSInstitute for Advanced Study, Einstein DriveUniversité de Paris, CNRS, Astroparticule et Cosmologie, F-75013 Paris, FranceINAF - Istituto di Radioastronomia, Istituto Nazionale di AstrofisicaINAF - Osservatorio di Astrofisica e Scienza dello Spazio, Istituto Nazionale di AstrofisicaINAF - Osservatorio di Astrofisica e Scienza dello Spazio di Bologna, Istituto Nazionale di AstrofisicaUniversity of Helsinki, Department of Physics, and Helsinki Institute of PhysicsINFN-Sezione di Roma TreINFN-Sezione di FerraraUniversit de ParisUniversit Claude Bernard Lyon 1INAF Osservatorio Astronomico di CapodimonteUniversit Lyon 1Instituto de Física Teórica, (UAM/CSIC)RWTH Aachen UniversityINAF Osservatorio Astrofisico di ArcetriUniversit degli Studi di MilanoINAF Osservatorio Astronomico di PadovaUniversit de MontpellierINAF Osservatorio di Astrofisica e Scienza dello Spazio di BolognaUniversit Di BolognaUniversit de Grenoble-AlpesINFN Sezione di TriesteINAF ` Osservatorio Astronomico di TriesteINFN Sezione di FirenzeNorwegian University of Science and TechnologyINAF Osservatorio Astronomico di BreraUniversity of Milano Bicocca
The Euclid mission of the European Space Agency will deliver weak gravitational lensing and galaxy clustering surveys that can be used to constrain the standard cosmological model and extensions thereof. We present forecasts from the combination of these surveys on the sensitivity to cosmological parameters including the summed neutrino mass MνM_\nu and the effective number of relativistic species NeffN_{\rm eff} in the standard Λ\LambdaCDM scenario and in a scenario with dynamical dark energy ($w_0 w_a$CDM). We compare the accuracy of different algorithms predicting the nonlinear matter power spectrum for such models. We then validate several pipelines for Fisher matrix and MCMC forecasts, using different theory codes, algorithms for numerical derivatives, and assumptions concerning the non-linear cut-off scale. The Euclid primary probes alone will reach a sensitivity of σ(Mν)=\sigma(M_\nu)=56meV in the Λ\LambdaCDM+MνM_\nu model, whereas the combination with CMB data from Planck is expected to achieve σ(Mν)=\sigma(M_\nu)=23meV and raise the evidence for a non-zero neutrino mass to at least the 2.6σ2.6\sigma level. This can be pushed to a 4σ4\sigma detection if future CMB data from LiteBIRD and CMB Stage-IV are included. In combination with Planck, Euclid will also deliver tight constraints on $\Delta N_{\rm eff}< 0.144(95 (95%CL) in the \LambdaCDM+CDM+M_\nu++N_{\rm eff}model,or model, or \Delta N_{\rm eff}< 0.063whenfutureCMBdataareincluded.Whenfloating when future CMB data are included. When floating (w_0, w_a),wefindthatthesensitivityto, we find that the sensitivity to N_{\rm eff}$ remains stable, while that to MνM_\nu degrades at most by a factor 2. This work illustrates the complementarity between the Euclid spectroscopic and imaging/photometric surveys and between Euclid and CMB constraints. Euclid will have a great potential for measuring the neutrino mass and excluding well-motivated scenarios with additional relativistic particles.
As a neurophysiological response to threat or adverse conditions, stress can affect cognition, emotion and behaviour with potentially detrimental effects on health in the case of sustained exposure. Since the affective content of speech is inherently modulated by an individual's physical and mental state, a substantial body of research has been devoted to the study of paralinguistic correlates of stress-inducing task load. Historically, voice stress analysis (VSA) has been conducted using conventional digital signal processing (DSP) techniques. Despite the development of modern methods based on deep neural networks (DNNs), accurately detecting stress in speech remains difficult due to the wide variety of stressors and considerable variability in the individual stress perception. To that end, we introduce a set of five datasets for task load detection in speech. The voice recordings were collected as either cognitive or physical stress was induced in the cohort of volunteers, with a cumulative number of more than a hundred speakers. We used the datasets to design and evaluate a novel self-supervised audio representation that leverages the effectiveness of handcrafted features (DSP-based) and the complexity of data-driven DNN representations. Notably, the proposed approach outperformed both extensive handcrafted feature sets and novel DNN-based audio representation learning approaches.
Causal discovery from observational data typically requires strong assumptions about the data-generating process. Previous research has established the identifiability of causal graphs under various models, including linear non-Gaussian, post-nonlinear, and location-scale models. However, these models may have limited applicability in real-world situations that involve a mixture of discrete and continuous variables or where the cause affects the variance or tail behavior of the effect. In this study, we introduce a new class of models, called Conditionally Parametric Causal Models (CPCM), which assume that the distribution of the effect, given the cause, belongs to well-known families such as Gaussian, Poisson, Gamma, or heavy-tailed Pareto distributions. These models are adaptable to a wide range of practical situations where the cause can influence the variance or tail behavior of the effect. We demonstrate the identifiability of CPCM by leveraging the concept of sufficient statistics. Furthermore, we propose an algorithm for estimating the causal structure from random samples drawn from CPCM. We evaluate the empirical properties of our methodology on various datasets, demonstrating state-of-the-art performance across multiple benchmarks.
Gravitational waves from black-hole merging events have revealed a population of extra-galactic BHs residing in short-period binaries with masses that are higher than expected based on most stellar evolution models - and also higher than known stellar-origin black holes in our Galaxy. It has been proposed that those high-mass BHs are the remnants of massive metal-poor stars. Gaia astrometry is expected to uncover many Galactic wide-binary systems containing dormant BHs, which may not have been detected before. The study of this population will provide new information on the BH-mass distribution in binaries and shed light on their formation mechanisms and progenitors. As part of the validation efforts in preparation for the fourth Gaia data release (DR4), we analysed the preliminary astrometric binary solutions, obtained by the Gaia Non-Single Star pipeline, to verify their significance and to minimise false-detection rates in high-mass-function orbital solutions. The astrometric binary solution of one source, Gaia BH3, implies the presence of a 32.70 \pm 0.82 M\odot BH in a binary system with a period of 11.6 yr. Gaia radial velocities independently validate the astrometric orbit. Broad-band photometric and spectroscopic data show that the visible component is an old, very metal-poor giant of the Galactic halo, at a distance of 590 pc. The BH in the Gaia BH3 system is more massive than any other Galactic stellar-origin BH known thus far. The low metallicity of the star companion supports the scenario that metal-poor massive stars are progenitors of the high-mass BHs detected by gravitational-wave telescopes. The Galactic orbit of the system and its metallicity indicate that it might belong to the Sequoia halo substructure. Alternatively, and more plausibly, it could belong to the ED-2 stream, which likely originated from a globular cluster that had been disrupted by the Milky Way.
CNRS logoCNRSCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of OsloChinese Academy of Sciences logoChinese Academy of SciencesUniversity of Manchester logoUniversity of ManchesterUniversity of ZurichUniversity College London logoUniversity College LondonUniversity of Oxford logoUniversity of OxfordUniversity of California, Irvine logoUniversity of California, IrvineUniversity of BonnUniversity of Copenhagen logoUniversity of CopenhagenUniversity of EdinburghTexas A&M University logoTexas A&M UniversityNASA Goddard Space Flight Center logoNASA Goddard Space Flight CenterRutherford Appleton LaboratoryUniversity of Southampton logoUniversity of SouthamptonJohns Hopkins University logoJohns Hopkins UniversityUniversité Paris-Saclay logoUniversité Paris-SaclayStockholm University logoStockholm UniversityUniversity of HelsinkiSorbonne Université logoSorbonne UniversitéUniversity of TurkuLeiden University logoLeiden UniversityUniversity of GenevaUniversity of PortsmouthUniversitat de BarcelonaUniversity of FerraraUniv LyonUniversity of SussexUniversité Côte d’AzurUniversità di TriesteDurham University logoDurham UniversityAix Marseille UniversityUniversity of CaliforniaJet Propulsion LaboratoryUniversity of Lyon 1Instituto de Astrofísica de CanariasEuropean Space AgencyUniversity of Cape TownThe University of Western AustraliaCNESJodrell Bank Centre for AstrophysicsUniversity of ValenciaFederal University of Rio de JaneiroUniversity of Hawai’iUniversity of KwaZulu-NatalThe University of ArizonaLudwig-Maximilians-UniversitätMax Planck Institute for AstronomyINAF Istituto di Astrofisica Spaziale e Fisica cosmica di MilanoINAF-Istituto di RadioastronomiaUniversité de MarseilleINAF – Osservatorio Astronomico di RomaInstitut d'Astrophysique de ParisInstitut de Física d’Altes Energies (IFAE)INAF-IASF MilanoDTU SpaceINAF-Osservatorio Astronomico di BolognaUniversité de LausanneCNRS-IN2P3Paris SaclayINAF - Osservatorio Astronomico di TorinoInstituto de Estudios Espaciales de Cataluña (IEEC)Dipartimento di Fisica e Astronomia, Università degli Studi di TriestePort d'Informació Científica (PIC)Universit Grenoble AlpesUniversit degli Studi di GenovaINAF Osservatorio Astronomico di CapodimonteUniversit degli Studi di PadovaUniversit Paris CitUniversit de LyonINAF Osservatorio Astrofisico di ArcetriINAF Osservatorio Astronomico di PadovaUniversit de MontpellierUniversity of Naples “Federico II”INAF Osservatorio di Astrofisica e Scienza dello Spazio di BolognaUniversit Di BolognaIFPU Institute for fundamental physics of the UniverseINFN Sezione di TriesteINAF ` Osservatorio Astronomico di TriesteINAF Osservatorio Astronomico di BreraUniversity of Milano Bicocca
We present the Flagship galaxy mock, a simulated catalogue of billions of galaxies designed to support the scientific exploitation of the Euclid mission. Euclid is a medium-class mission of the European Space Agency optimised to determine the properties of dark matter and dark energy on the largest scales of the Universe. It probes structure formation over more than 10 billion years primarily from the combination of weak gravitational lensing and galaxy clustering data. The breath of Euclid's data will also foster a wide variety of scientific analyses. The Flagship simulation was developed to provide a realistic approximation to the galaxies that will be observed by Euclid and used in its scientific analyses. We ran a state-of-the-art N-body simulation with four trillion particles, producing a lightcone on the fly. From the dark matter particles, we produced a catalogue of 16 billion haloes in one octant of the sky in the lightcone up to redshift z=3. We then populated these haloes with mock galaxies using a halo occupation distribution and abundance matching approach, calibrating the free parameters of the galaxy mock against observed correlations and other basic galaxy properties. Modelled galaxy properties include luminosity and flux in several bands, redshifts, positions and velocities, spectral energy distributions, shapes and sizes, stellar masses, star formation rates, metallicities, emission line fluxes, and lensing properties. We selected a final sample of 3.4 billion galaxies with a magnitude cut of H_E<26, where we are complete. We have performed a comprehensive set of validation tests to check the similarity to observational data and theoretical models. In particular, our catalogue is able to closely reproduce the main characteristics of the weak lensing and galaxy clustering samples to be used in the mission's main cosmological analysis. (abridged)
ETH Zurich logoETH ZurichCNRS logoCNRSCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of Illinois at Urbana-Champaign logoUniversity of Illinois at Urbana-ChampaignUniversity of OsloChinese Academy of Sciences logoChinese Academy of SciencesUniversity College London logoUniversity College LondonUniversity of Oxford logoUniversity of OxfordUniversity of California, Irvine logoUniversity of California, IrvineUniversity of Copenhagen logoUniversity of CopenhagenUniversity of EdinburghETH Zürich logoETH ZürichUniversity of British Columbia logoUniversity of British ColumbiaUniversity of CreteUniversidade de LisboaSpace Telescope Science Institute logoSpace Telescope Science InstituteImperial CollegeUniversity of Southampton logoUniversity of SouthamptonInstitute for Advanced StudyUniversité Paris-Saclay logoUniversité Paris-SaclayStockholm University logoStockholm UniversityUniversity of HelsinkiUniversité de GenèveSorbonne Université logoSorbonne UniversitéUniversity of HertfordshireTampere UniversityUniversity of GenevaUniversity of PortsmouthUniversity of IcelandUniversità di Milano-BicoccaUniversity of SussexINAF - Osservatorio Astrofisico di TorinoUniversité Côte d’AzurUniversidade Federal do Rio de JaneiroDurham University logoDurham UniversityINAFNiels Bohr InstituteUniversity of CaliforniaUniversity of JyväskyläUniversity of PadovaUniversity of LiègeInstituto de Astrofísica de CanariasUniversity of NottinghamEuropean Space AgencyEuropean Southern Observatory logoEuropean Southern ObservatorySISSAUniversity of TriesteJodrell Bank Centre for AstrophysicsOsservatorio Astrofisico di ArcetriCentro de Investigaciones Energéticas, Medioambientales y TecnológicasUniversità di Napoli Federico IIUniversity of California, Santa Cruz logoUniversity of California, Santa CruzUniversity of KwaZulu-NatalLudwig-Maximilians-UniversitätScience and Technology Facilities CouncilINAF – Istituto di Astrofisica e Planetologia SpazialiUniversity of the Western CapeINAF Istituto di Astrofisica Spaziale e Fisica cosmica di MilanoLaboratoire d’Astrophysique de MarseilleUniversité de Paris-SaclayMax-Planck Institut für extraterrestrische PhysikINAF-Istituto di RadioastronomiaArgelander-Institut für Astronomie der Universität BonnINAF – Osservatorio Astronomico di RomaInstitut d'Astrophysique de ParisInstitut de Física d’Altes Energies (IFAE)LIPUniversity of RomeInstitut d’Astrophysique SpatialeIN2P3/CNRSDTU SpaceUniversité d’Aix-MarseilleINAF-Osservatorio Astronomico di BolognaINAF-IASFUniversité de LausanneINAF-OASParis SaclayINAF-OATCosmic Dawn Center(DAWN)Institute of Space Sciences (ICE–CSIC)Universit de ParisUniversit di FerraraINAF Osservatorio Astronomico di CapodimonteUniversit Paris CitUniversit de StrasbourgUniversit de LyonINAF Osservatorio Astronomico di PadovaUniversit degli Studi di TorinoUniversity of Naples “Federico II”INAF Osservatorio di Astrofisica e Scienza dello Spazio di BolognaUniversit Di BolognaINAF ` Osservatorio Astronomico di TriesteINAF IRAUniversit degli Studi Roma TreINAF Osservatorio Astronomico di Brera
Euclid will cover over 14000 deg2deg^{2} with two optical and near-infrared spectro-photometric instruments, and is expected to detect around ten million active galactic nuclei (AGN). This unique data set will make a considerable impact on our understanding of galaxy evolution and AGN. In this work we identify the best colour selection criteria for AGN, based only on Euclid photometry or including ancillary photometric observations, such as the data that will be available with the Rubin legacy survey of space and time (LSST) and observations already available from Spitzer/IRAC. The analysis is performed for unobscured AGN, obscured AGN, and composite (AGN and star-forming) objects. We make use of the spectro-photometric realisations of infrared-selected targets at all-z (SPRITZ) to create mock catalogues mimicking both the Euclid Wide Survey (EWS) and the Euclid Deep Survey (EDS). Using these catalogues we estimate the best colour selection, maximising the harmonic mean (F1) of completeness and purity. The selection of unobscured AGN in both Euclid surveys is possible with Euclid photometry alone with F1=0.22-0.23, which can increase to F1=0.43-0.38 if we limit at z>0.7. Such selection is improved once the Rubin/LSST filters (a combination of the u, g, r, or z filters) are considered, reaching F1=0.84 and 0.86 for the EDS and EWS, respectively. The combination of a Euclid colour with the [3.6]-[4.5] colour, which is possible only in the EDS, results in an F1-score of 0.59, improving the results using only Euclid filters, but worse than the selection combining Euclid and LSST. The selection of composite (fAGNf_{\rm AGN}=0.05-0.65 at 8-40 μm\mu m) and obscured AGN is challenging, with F1<0.3 even when including ancillary data. This is driven by the similarities between the broad-band spectral energy distribution of these AGN and star-forming galaxies in the wavelength range 0.3-5 μm\mu m.
We consider the problem of learning a set of direct causes of a target variable from an observational joint distribution. Learning directed acyclic graphs (DAGs) that represent the causal structure is a fundamental problem in science. Several results are known when the full DAG is identifiable from the distribution, such as assuming a nonlinear Gaussian data-generating process. Here, we are only interested in identifying the direct causes of one target variable (local causal structure), not the full DAG. This allows us to relax the identifiability assumptions and develop possibly faster and more robust algorithms. In contrast to the Invariance Causal Prediction framework, we only assume that we observe one environment without any interventions. We discuss different assumptions for the data-generating process of the target variable under which the set of direct causes is identifiable from the distribution. While doing so, we put essentially no assumptions on the variables other than the target variable. In addition to the novel identifiability results, we provide two practical algorithms for estimating the direct causes from a finite random sample and demonstrate their effectiveness on several benchmark and real datasets.
Academia SinicaCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of OsloUniversity of Cambridge logoUniversity of CambridgeChinese Academy of Sciences logoChinese Academy of SciencesUniversity of Manchester logoUniversity of ManchesterUniversity of Southern California logoUniversity of Southern CaliforniaUniversity of Oxford logoUniversity of OxfordUniversity of California, Irvine logoUniversity of California, IrvineUniversity of BonnUniversity of Copenhagen logoUniversity of CopenhagenThe University of EdinburghUniversity of LjubljanaSokendaiETH Zürich logoETH ZürichUniversity of CreteUniversity of Texas at Austin logoUniversity of Texas at AustinUniversity of GranadaUniversity of the Basque Country (UPV/EHU)Université Paris-Saclay logoUniversité Paris-SaclayUniversity of HelsinkiUniversity of ZagrebUniversité de GenèveAalto University logoAalto UniversityCEA logoCEAUniversity of GenevaUniversity of PortsmouthUniversity of FerraraMax Planck Institute for AstrophysicsUniversity of SussexUniversity of TartuINAF - Osservatorio Astrofisico di TorinoUniversity of FlorenceUniversity of JyväskyläUniversity of PadovaInstituto de Astrofísica de CanariasUniversity of NottinghamEuropean Space AgencySISSA — International School for Advanced StudiesUniversity of TriesteUniversity of LisbonINFN, Sezione di TorinoUniversity of Hawai’iUniversity of KwaZulu-NatalUniversity of California RiversideUniversity of the Western CapeUniversity of BarcelonaNational Observatory of AthensLaboratoire d’Astrophysique de MarseilleKavli IPMU (WPI), UTIAS, The University of TokyoINAF-Istituto di RadioastronomiaINAF - Osservatorio di Astrofisica e Scienza dello SpazioINAF – Osservatorio Astronomico di RomaInstitut d’Estudis Espacials de Catalunya (IEEC)INFN - Sezione di PadovaINAF - Osservatorio Astronomico di ArcetriInstitute for Astronomy, University of HawaiiINAF-IASF MilanoKapteyn Astronomical Institute, University of GroningenLudwig Maximilians UniversityInstitut d’Astrophysique SpatialeThe Oskar Klein Centre for Cosmoparticle PhysicsDTU SpaceCRAL, Observatoire de LyonUniversity of AarhusINFN-Sezione di BolognaINFN Sezione di RomaINAF-Osservatorio Astronomico di BolognaLeiden ObservatoryUniversité de LausanneUniversity of StockholmUniversité de ProvenceFinnish Centre for Astronomy with ESO (FINCA)Laboratoire de Physique Subatomique et de CosmologieBarcelona Institute of Science and TechnologyAIM, CEA, CNRS, Université Paris-SaclayInstituto de Astrofísica e Ciências do Espaço, Universidade de LisboaWarsaw University ObservatoryNOVA Optical Infrared Instrumentation Group at ASTRONInstitute for Theoretical Physics, University of ZurichInstitute of Theoretical Astrophysics, University of OsloAstronomical Observatory of BelgradeNAOJDARK Cosmology CentreIRAP, Université de Toulouse, CNRS, CNESInstitute for Advanced Study, University of AmsterdamDanish Space Research InstituteDepartment of Physics & Astronomy, University of SussexInfrared Processing and Analysis Center, CaltechAPC, UMR 7164, CNRS, Université Paris Diderot-ParisINFN-Sezione di FerraraInstitute of Space Sciences (ICE–CSIC)Universit de ParisJodrell Bank Centre for Astrophysics The University of ManchesterINAF Osservatorio Astronomico di CapodimonteUniversit de StrasbourgMax Planck-Institute for Extraterrestrial PhysicsUniversit de LyonINAF Osservatorio Astronomico di PadovaUniversit de MontpellierINAF Osservatorio di Astrofisica e Scienza dello Spazio di BolognaINFN Sezione di TriesteINAF ` Osservatorio Astronomico di TriesteExcellence Cluster 'Universe'INAF Osservatorio Astronomico di BreraUniversity of Milano Bicocca
Euclid will provide deep NIR imaging to \sim26.5 AB magnitude over \sim59 deg2^2 in its deep and auxiliary fields. The Cosmic DAWN survey complements the deep Euclid data with matched depth multiwavelength imaging and spectroscopy in the UV--IR to provide consistently processed Euclid selected photometric catalogs, accurate photometric redshifts, and measurements of galaxy properties to a redshift of z10z\sim 10. In this paper, we present an overview of the survey, including the footprints of the survey fields, the existing and planned observations, and the primary science goals for the combined data set.
The Near-Infrared Spectrometer and Photometer (NISP) on board the Euclid satellite provides multiband photometry and R>=450 slitless grism spectroscopy in the 950-2020nm wavelength range. In this reference article we illuminate the background of NISP's functional and calibration requirements, describe the instrument's integral components, and provide all its key properties. We also sketch the processes needed to understand how NISP operates and is calibrated, and its technical potentials and limitations. Links to articles providing more details and technical background are included. NISP's 16 HAWAII-2RG (H2RG) detectors with a plate scale of 0.3" pix^-1 deliver a field-of-view of 0.57deg^2. In photo mode, NISP reaches a limiting magnitude of ~24.5AB mag in three photometric exposures of about 100s exposure time, for point sources and with a signal-to-noise ratio (SNR) of 5. For spectroscopy, NISP's point-source sensitivity is a SNR = 3.5 detection of an emission line with flux ~2x10^-16erg/s/cm^2 integrated over two resolution elements of 13.4A, in 3x560s grism exposures at 1.6 mu (redshifted Ha). Our calibration includes on-ground and in-flight characterisation and monitoring of detector baseline, dark current, non-linearity, and sensitivity, to guarantee a relative photometric accuracy of better than 1.5%, and relative spectrophotometry to better than 0.7%. The wavelength calibration must be better than 5A. NISP is the state-of-the-art instrument in the NIR for all science beyond small areas available from HST and JWST - and an enormous advance due to its combination of field size and high throughput of telescope and instrument. During Euclid's 6-year survey covering 14000 deg^2 of extragalactic sky, NISP will be the backbone for determining distances of more than a billion galaxies. Its NIR data will become a rich reference imaging and spectroscopy data set for the coming decades.
University of CanterburyCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of OsloUCLA logoUCLASun Yat-Sen University logoSun Yat-Sen UniversityUniversity of Manchester logoUniversity of ManchesterUniversity of Southern California logoUniversity of Southern CaliforniaTel Aviv University logoTel Aviv UniversityGhent UniversityUniversity College London logoUniversity College LondonUniversity of Oxford logoUniversity of OxfordNikhefUniversity of California, Irvine logoUniversity of California, IrvineUniversity of Bristol logoUniversity of BristolUniversity of Copenhagen logoUniversity of CopenhagenUniversity of EdinburghETH Zürich logoETH ZürichYonsei UniversityTexas A&M University logoTexas A&M UniversityUniversity of British Columbia logoUniversity of British ColumbiaNASA Goddard Space Flight Center logoNASA Goddard Space Flight CenterUniversidade de LisboaUniversity of Southampton logoUniversity of SouthamptonUniversité Paris-Saclay logoUniversité Paris-SaclayStockholm University logoStockholm UniversityUniversity of HelsinkiKing’s College London logoKing’s College LondonThe University of SydneyUniversity of ZagrebUniversité de GenèveSorbonne Université logoSorbonne UniversitéUniversity of LeidenUniversity of PortsmouthUniversity of IcelandUniversity of SussexObservatoire de ParisUniversité de LiègeINAF - Osservatorio Astrofisico di TorinoInstituto de Astrofísica e Ciências do EspaçoNiels Bohr InstituteInstituto de Astrofísica de CanariasUniversity of the WitwatersrandUniversity of NottinghamSISSAPontificia Universidad Católica de ChileUniversidad de ValparaísoJodrell Bank Centre for AstrophysicsShanghai Astronomical ObservatoryUniversidad de CantabriaUniversity of Hawai’iUniversity of KwaZulu-NatalLudwig-Maximilians-UniversitätInstituto de Astrofísica de Andalucía-CSICUniversity of the Western CapeLaboratoire d’Astrophysique de MarseilleESRF - The European SynchrotronMax-Planck Institut für extraterrestrische PhysikINAF-Istituto di RadioastronomiaUniversidad Autonoma de MadridINAF – Osservatorio Astronomico di RomaInstitut d'Astrophysique de ParisInstitut de Física d’Altes Energies (IFAE)Canadian Institute for Theoretical AstrophysicsDeutsches Elektronen SynchrotronIPAC, California Institute of TechnologyINAF- Osservatorio Astronomico di CagliariINAF-IASF MilanoUniversità di FirenzeNetherlands Institute for Space ResearchUniversitäts-Sternwarte MünchenDTU SpaceINAF-OAS BolognaINFN-Sezione di BolognaUniversità di RomaAPC, UMR 7164, Université Paris DiderotINAF-Osservatorio Astronomico di BolognaUniversité de LausanneUniversité de ProvenceDipartimento di Fisica e Astronomia, Università di BolognaIRAP-CNRSUniversité Paris-Saclay, CNRSIstituto Nazionale di Fisica Nucleare, Sezione di FerraraAix Marseille Université, CNRS, CNESESAC/ESACNRS, IRAP, UMR 5277, Toulouse, FranceUniversité de Genève, Observatoire de GenèveIPhT, CEAICC University of BarcelonaIstituto Nazionale di Fisica Nucleare Sezione di TorinoUniversit de ParisUniversit Grenoble AlpesUniversit degli Studi di GenovaUniversit de ToulouseUniversit Claude Bernard Lyon 1INAF Osservatorio Astronomico di CapodimonteUniversit de BordeauxUniversit Paris CitUniversit de StrasbourgUniversit de LyonUniversit di PadovaINAF Osservatorio Astrofisico di ArcetriUniversit de MontpellierINAF Osservatorio di Astrofisica e Scienza dello Spazio di BolognaINFN Sezione di TriesteINAF ` Osservatorio Astronomico di TriesteUniversit degli Studi Roma TreINAF Osservatorio Astronomico di Brera
We present the results of the single-component Sérsic profile fitting for the magnitude-limited sample of \IE&lt;23 galaxies within the 63.1 deg2^2 area of the Euclid Quick Data Release (Q1). The associated morphological catalogue includes two sets of structural parameters fitted using \texttt{SourceXtractor++}: one for VIS \IE images and one for a combination of three NISP images in \YE, \JE and \HE bands. We compare the resulting Sérsic parameters to other morphological measurements provided in the Q1 data release, and to the equivalent parameters based on higher-resolution \HST imaging. These comparisons confirm the consistency and the reliability of the fits to Q1 data. Our analysis of colour gradients shows that NISP profiles have systematically smaller effective radii (ReR_{\rm e}) and larger Sérsic indices (nn) than in VIS. In addition, we highlight trends in NISP-to-VIS parameter ratios with both magnitude and nVISn_{\rm VIS}. From the 2D bimodality of the (ur)(u-r) colour-log(n)\log(n) plane, we define a (ur)lim(n)(u-r)_{\rm lim}(n) that separates early- and late-type galaxies (ETGs and LTGs). We use the two subpopulations to examine the variations of nn across well-known scaling relations at z&lt;1. ETGs display a steeper size--stellar mass relation than LTGs, indicating a difference in the main drivers of their mass assembly. Similarly, LTGs and ETGs occupy different parts of the stellar mass--star-formation rate plane, with ETGs at higher masses than LTGs, and further down below the Main Sequence of star-forming galaxies. This clear separation highlights the link known between the shutdown of star formation and morphological transformations in the Euclid imaging data set. In conclusion, our analysis demonstrates both the robustness of the Sérsic fits available in the Q1 morphological catalogue and the wealth of information they provide for studies of galaxy evolution with Euclid.
Backdoor attacks allow an attacker to embed a specific vulnerability in a machine learning algorithm, activated when an attacker-chosen pattern is presented, causing a specific misprediction. The need to identify backdoors in biometric scenarios has led us to propose a novel technique with different trade-offs. In this paper we propose to use model pairs on open-set classification tasks for detecting backdoors. Using a simple linear operation to project embeddings from a probe model's embedding space to a reference model's embedding space, we can compare both embeddings and compute a similarity score. We show that this score, can be an indicator for the presence of a backdoor despite models being of different architectures, having been trained independently and on different datasets. This technique allows for the detection of backdoors on models designed for open-set classification tasks, which is little studied in the literature. Additionally, we show that backdoors can be detected even when both models are backdoored. The source code is made available for reproducibility purposes.
California Institute of Technology logoCalifornia Institute of TechnologyUniversity of OsloUniversity of VictoriaUniversity of Southern California logoUniversity of Southern CaliforniaUniversity College London logoUniversity College LondonUniversity of Oxford logoUniversity of OxfordUniversity of Science and Technology of China logoUniversity of Science and Technology of ChinaUniversity of California, Irvine logoUniversity of California, IrvineUniversity of Copenhagen logoUniversity of CopenhagenUniversity of EdinburghINFN logoINFNETH Zürich logoETH ZürichUniversity of CreteUniversity of the AegeanUniversity of Pennsylvania logoUniversity of PennsylvaniaUniversité Paris-Saclay logoUniversité Paris-SaclayHelsinki Institute of PhysicsStockholm University logoStockholm UniversityUniversity of HelsinkiUniversité de GenèveUniversity of PortsmouthConsejo Superior de Investigaciones CientíficasUniversità di GenovaUniversidade do PortoUniversity of SussexMax-Planck-Institut für AstrophysikUniversità di TriesteINAFInstituto de Astrofísica de CanariasUniversity of NottinghamThe University of Western AustraliaEuropean Southern Observatory logoEuropean Southern ObservatoryIstituto Nazionale di AstrofisicaUniversità di Napoli Federico IIUniversity of KwaZulu-NatalLudwig-Maximilians-UniversitätKapteyn Astronomical InstituteINAF – Istituto di Astrofisica Spaziale e Fisica Cosmica MilanoUniversité de MarseilleINAF – Osservatorio Astronomico di RomaLeibniz-Institut für Astrophysik PotsdamUniversité Claude Bernard LyonINAF-IASF MilanoUniversità di FirenzeInstitut d’Astrophysique SpatialeIRAPDTU SpaceArgelander-Institut für AstronomieRheinische Friedrich-Wilhelms-Universität BonnNational Astronomical Observatories of ChinaUniversité de LausanneInstitute for Theoretical PhysicsINAF - Osservatorio Astronomico di TorinoIPMULisbon UniversityOsservatorio Astrofisico di CataniaNAOCINAF-IASF, BolognaUniversit de ParisExcellence Cluster ‘Origins’Universit Paris CitUniversit de StrasbourgUniversit de LyonUniversit di TorinoINAF Osservatorio Astronomico di PadovaUniversit de MontpellierINAF Osservatorio di Astrofisica e Scienza dello Spazio di BolognaUniversit Di BolognaINAF ` Osservatorio Astronomico di TriesteUniversit degli Studi Roma TreINAF Osservatorio Astronomico di Brera
LensMC is a weak lensing shear measurement method developed for Euclid and Stage-IV surveys. It is based on forward modelling in order to deal with convolution by a point spread function (PSF) with comparable size to many galaxies; sampling the posterior distribution of galaxy parameters via Markov Chain Monte Carlo; and marginalisation over nuisance parameters for each of the 1.5 billion galaxies observed by Euclid. We quantified the scientific performance through high-fidelity images based on the Euclid Flagship simulations and emulation of the Euclid VIS images; realistic clustering with a mean surface number density of 250 arcmin2^{-2} (I_{\rm E}&lt;29.5) for galaxies, and 6 arcmin2^{-2} (I_{\rm E}&lt;26) for stars; and a diffraction-limited chromatic PSF with a full width at half maximum of 0. ⁣20.^{\!\prime\prime}2 and spatial variation across the field of view. LensMC measured objects with a density of 90 arcmin2^{-2} (I_{\rm E}&lt;26.5) in 4500 deg2^2. The total shear bias was broken down into measurement (our main focus here) and selection effects (which will be addressed elsewhere). We found measurement multiplicative and additive biases of m1=(3.6±0.2)×103m_1=(-3.6\pm0.2)\times10^{-3}, m2=(4.3±0.2)×103m_2=(-4.3\pm0.2)\times10^{-3}, c1=(1.78±0.03)×104c_1=(-1.78\pm0.03)\times10^{-4}, c2=(0.09±0.03)×104c_2=(0.09\pm0.03)\times10^{-4}; a large detection bias with a multiplicative component of 1.2×1021.2\times10^{-2} and an additive component of 3×104-3\times10^{-4}; and a measurement PSF leakage of α1=(9±3)×104\alpha_1=(-9\pm3)\times10^{-4} and α2=(2±3)×104\alpha_2=(2\pm3)\times10^{-4}. When model bias is suppressed, the obtained measurement biases are close to Euclid requirement and largely dominated by undetected faint galaxies (5×103-5\times10^{-3}). Although significant, model bias will be straightforward to calibrate given the weak sensitivity. LensMC is publicly available at this https URL
ETH Zurich logoETH ZurichCNRS logoCNRSCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of OsloUniversity of Cambridge logoUniversity of CambridgeUniversity of Waterloo logoUniversity of WaterlooUniversity of Chicago logoUniversity of ChicagoUniversity College London logoUniversity College LondonUniversity of Oxford logoUniversity of OxfordUniversity of California, Irvine logoUniversity of California, IrvineUniversity of Copenhagen logoUniversity of CopenhagenUniversity of EdinburghCornell University logoCornell UniversityNASA Goddard Space Flight Center logoNASA Goddard Space Flight CenterUniversidade de LisboaEPFL logoEPFLUniversity of GenoaUniversidad Autónoma de MadridUniversité Paris-Saclay logoUniversité Paris-SaclayHelsinki Institute of PhysicsUniversity of HelsinkiPerimeter Institute for Theoretical Physics logoPerimeter Institute for Theoretical PhysicsUniversité de GenèveSorbonne Université logoSorbonne UniversitéUniversity of HertfordshireUniversity of TurkuUniversity of PortsmouthLudwig-Maximilians-Universität MünchenUniversidad Complutense de MadridUniversity of St Andrews logoUniversity of St AndrewsUniversity of SussexObservatoire de ParisTechnical University of DenmarkINAF - Osservatorio Astrofisico di TorinoDurham University logoDurham UniversityUniversity of Groningen logoUniversity of GroningenInstituto de Astrofísica e Ciências do EspaçoJet Propulsion LaboratoryUniversity of Southern DenmarkInstituto de Astrofísica de CanariasBandung Institute of TechnologyRuhr-Universität BochumSISSAINFN, Sezione di TorinoPontificia Universidad Católica de ChileUniversidad de La LagunaConsejo Superior de Investigaciones Científicas (CSIC)University of Hawai’iINFN, Sezione di MilanoEuropean Space Astronomy Centre (ESAC)Max Planck Institute for AstronomyCNRS/IN2P3INAF – Osservatorio Astronomico di RomaInstitut d'Astrophysique de ParisUniversidad de SalamancaInstitut de Física d’Altes Energies (IFAE)Institut d’Estudis Espacials de Catalunya (IEEC)Institució Catalana de Recerca i Estudis AvançatsUniversità della CalabriaUniversità degli Studi di Roma "Tor Vergata"INFN - Sezione di PadovaINAF- Osservatorio Astronomico di CagliariINAF-IASF MilanoUniversità di FirenzeInstitute of Space ScienceTelespazio U.K. Ltd.LAMDTU SpaceEuropean Space Agency (ESA)INFN-Sezione di BolognaUniversidad Politécnica de CartagenaAstroparticule et CosmologieRuprecht-Karls-Universität HeidelbergCentro de Estudios de Física del Cosmos de Aragón (CEFCA)CPPMUniversité de LausanneInfrared Processing and Analysis CenterLERMAInstitut d’Astrophysique Spatiale (IAS)Agenzia Spaziale Italiana (ASI)Instituto de Física Teórica UAM/CSICINAF, Istituto di Astrofisica Spaziale e Fisica Cosmica di BolognaUniversité LyonIP2I LyonInstituto de Física de Partículas y del Cosmos IPARCOSINAF – OAS, Osservatorio di Astrofisica e Scienza dello Spazio di BolognaLaboratoire de Physique de Clermont (LPC)CEA/DRFArgelander-Institut für Astronomie (AIfA)Port d'Informació Científica (PIC)ITERA Research InstituteSpace SystemsCosmic Dawn Center(DAWN)Institute of Space Sciences (ICE–CSIC)INFN National Institute for Nuclear PhysicsUniversit de ParisUniversit Claude Bernard Lyon 1INAF Osservatorio Astronomico di CapodimonteAix-Marseille Universit",Universit degli Studi di PadovaExcellence Cluster ‘Origins’Universit Paris CitMax Planck-Institute for Extraterrestrial PhysicsUniversit Clermont AuvergneUniversit degli Studi di MilanoINAF Osservatorio Astronomico di PadovaUniversit degli Studi di TorinoUniversity of Naples “Federico II”Center for Astrophysics  Harvard & SmithsonianUniversit Di BolognaIFPU Institute for fundamental physics of the UniverseINFN Sezione di TriesteINAF ` Osservatorio Astronomico di TriesteINAF IRAUniversit degli Studi di TriesteINAF Osservatorio Astronomico di Brera
We investigate the accuracy and range of validity of the perturbative model for the 2-point (2PCF) and 3-point (3PCF) correlation functions in real space in view of the forthcoming analysis of the Euclid mission spectroscopic sample. We take advantage of clustering measurements from four snapshots of the Flagship I N-body simulations at z = {0.9, 1.2, 1.5, 1.8}, which mimic the expected galaxy population in the ideal case of absence of observational effects such as purity and completeness. For the 3PCF we consider all available triangle configurations given a minimal separation. First, we assess the model performance by fixing the cosmological parameters and evaluating the goodness-of-fit provided by the perturbative bias expansion in the joint analysis of the two statistics, finding overall agreement with the data down to separations of 20 Mpc/h. Subsequently, we build on the state-of-the-art and extend the analysis to include the dependence on three cosmological parameters: the amplitude of scalar perturbations As, the matter density {\omega}cdm and the Hubble parameter h. To achieve this goal, we develop an emulator capable of generating fast and robust modelling predictions for the two summary statistics, allowing efficient sampling of the joint likelihood function. We therefore present the first joint full-shape analysis of the real-space 2PCF and 3PCF, testing the consistency and constraining power of the perturbative model across both probes, and assessing its performance in a combined likelihood framework. We explore possible systematic uncertainties induced by the perturbative model at small scales finding an optimal scale cut of rmin = 30 Mpc/h for the 3PCF, when imposing an additional limitation on nearly isosceles triangular configurations included in the data vector. This work is part of a Euclid Preparation series validating theoretical models for galaxy clustering.
We present an analysis of globular clusters (GCs) of dwarf galaxies in the Perseus galaxy cluster to explore the relationship between dwarf galaxy properties and their GCs. Our focus is on GC numbers (NGCN_{\rm GC}) and GC half-number radii (RGCR_{\rm GC}) around dwarf galaxies, and their relations with host galaxy stellar masses (MM_*), central surface brightnesses (μ0\mu_0), and effective radii (ReR_{\rm e}). Interestingly, we find that at a given stellar mass, RGCR_{\rm GC} is almost independent of the host galaxy μ0\mu_0 and ReR_{\rm e}, while RGC/ReR_{\rm GC}/R_{\rm e} depends on μ0\mu_0 and ReR_{\rm e}; lower surface brightness and diffuse dwarf galaxies show RGC/Re1R_{\rm GC}/R_{\rm e}\approx 1 while higher surface brightness and compact dwarf galaxies show RGC/Re1.5R_{\rm GC}/R_{\rm e}\approx 1.5-22. This means that for dwarf galaxies of similar stellar mass, the GCs have a similar median extent; however, their distribution is different from the field stars of their host. Additionally, low surface brightness and diffuse dwarf galaxies on average have a higher NGCN_{\rm GC} than high surface brightness and compact dwarf galaxies at any given stellar mass. We also find that UDGs (ultra-diffuse galaxies) and non-UDGs have similar RGCR_{\rm GC}, while UDGs have smaller RGC/ReR_{\rm GC}/R_{\rm e} (typically less than 1) and 3-4 times higher NGCN_{\rm GC} than non-UDGs. Examining nucleated and not-nucleated dwarf galaxies, we find that for M_*&gt;10^8M_{\odot}, nucleated dwarf galaxies seem to have smaller RGCR_{\rm GC} and RGC/ReR_{\rm GC}/R_{\rm e}, with no significant differences between their NGCN_{\rm GC}, except at M_*&lt;10^8M_{\odot} where the nucleated dwarf galaxies tend to have a higher NGCN_{\rm GC}. Lastly, we explore the stellar-to-halo mass ratio (SHMR) of dwarf galaxies and conclude that the Perseus cluster dwarf galaxies follow the expected SHMR at z=0z=0 extrapolated down to M=106MM_*=10^6M_{\odot}.
University of Toronto logoUniversity of TorontoCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of Pittsburgh logoUniversity of PittsburghUniversity of OsloUniversity of VictoriaUniversity of ZurichUC Berkeley logoUC BerkeleyUniversity of Oxford logoUniversity of OxfordUniversity of California, Irvine logoUniversity of California, IrvineUniversity of BonnScuola Normale SuperioreUniversity of Copenhagen logoUniversity of CopenhagenUniversity of EdinburghETH Zürich logoETH ZürichTexas A&M University logoTexas A&M UniversityCSICNASA Goddard Space Flight Center logoNASA Goddard Space Flight CenterUniversity of Florida logoUniversity of FloridaINFN Sezione di PisaUniversity of GranadaUniversität HeidelbergUniversity of Minnesota logoUniversity of MinnesotaUniversité Paris-Saclay logoUniversité Paris-SaclayStockholm University logoStockholm UniversityUniversity of HelsinkiKing’s College London logoKing’s College LondonUniversity of Arizona logoUniversity of ArizonaUniversity of ZagrebUniversité de GenèveInstituto de Física Teórica UAM-CSICUniversity of BolognaLeiden University logoLeiden UniversityUniversity of GenevaUniversity of PortsmouthMoscow Institute of Physics and TechnologyUniversity of SussexObservatoire de ParisUniversity of BirminghamNordita, KTH Royal Institute of Technology and Stockholm UniversityUniversity of Groningen logoUniversity of GroningenINAFUniversity of JyväskyläInstituto de Astrofísica de CanariasUniversity of the WitwatersrandUniversity of NottinghamEuropean Space AgencyUniversity of Cape TownSISSACNESUniversity of TriesteINFN, Sezione di TorinoPontificia Universidad Católica de ChileUniversidad de ValparaísoObservatoire de la Côte d’AzurUniversity of Hawai’iINFN, Sezione di MilanoUniversity of KwaZulu-NatalLudwig-Maximilians-UniversitätUniversity of California RiversideUniversity of the Western CapeIndian Institute of Technology IndoreUniversidad de AtacamaINAF – Osservatorio Astronomico di RomaInstitut d’Estudis Espacials de Catalunya (IEEC)Università degli Studi di Roma "Tor Vergata"INFN - Sezione di PadovaUniversity of BucharestINAF-IASF MilanoUniversity of RomeAix Marseille Université, CNRS, CNES, LAMDTU SpaceINFN-Sezione di BolognaINFN Sezione di RomaUniversité de LausanneAIM, CEA, CNRS, Université Paris-SaclayInstituto de Astrofísica e Ciências do Espaço, Universidade de LisboaDipartimento di Fisica e Astronomia, Alma Mater Studiorum - Università di BolognaDipartimento di Fisica - Sezione di Astronomia, Università di TriesteAPC, UMR 7164, CNRS, Université Paris DiderotInstitut d’Optique Graduate School, Université Paris-SaclayGEPI, Observatoire de Paris, Université PSLUniv Lyon, UCAUniversitet i OsloINFN-Sezione di Roma TreUniversit de ParisUniversit Grenoble AlpesUniversit de ToulouseUniversit Claude Bernard Lyon 1Universit di FerraraINAF Osservatorio Astronomico di CapodimonteUniversit de StrasbourgMax Planck-Institute for Extraterrestrial PhysicsRuhr-University-BochumINAF Osservatorio Astrofisico di ArcetriINAF Osservatorio Astronomico di PadovaUniversit de MontpellierUniversit degli Studi di Napoli Federico IIINAF Osservatorio di Astrofisica e Scienza dello Spazio di BolognaIFPU Institute for fundamental physics of the UniverseINFN Sezione di TriesteUniversit degli Studi Roma Tre
The intracluster light (ICL) permeating galaxy clusters is a tracer of the cluster's assembly history, and potentially a tracer of their dark matter structure. In this work we explore the capability of the Euclid Wide Survey to detect ICL using H-band mock images. We simulate clusters across a range of redshifts (0.3-1.8) and halo masses (1013.910^{13.9}-1015.010^{15.0} M_\odot), using an observationally motivated model of the ICL. We identify a 50-200 kpc circular annulus around the brightest cluster galaxy (BCG) in which the signal-to-noise ratio (S/N) of the ICL is maximised and use the S/N within this aperture as our figure of merit for ICL detection. We compare three state-of-the-art methods for ICL detection, and find that a method that performs simple aperture photometry after high-surface brightness source masking is able to detect ICL with minimal bias for clusters more massive than 1014.210^{14.2} M_\odot. The S/N of the ICL detection is primarily limited by the redshift of the cluster, driven by cosmological dimming, rather than the mass of the cluster. Assuming the ICL in each cluster contains 15% of the stellar light, we forecast that Euclid will be able to measure the presence of ICL in up to 80000\sim80000 clusters of &gt;10^{14.2} M_\odot between z=0.3z=0.3 and 1.5 with a S/N&gt;3. Half of these clusters will reside below z=0.75z=0.75 and the majority of those below z=0.6z=0.6 will be detected with a S/N &gt;20. A few thousand clusters at 1.31014.71.310^{14.7} M_\odot. Euclid will detect the ICL at more than 500 kpc distance from the BCG, up to z=0.7z=0.7, in several hundred of these massive clusters over its large survey volume.
We report the first observation of the charmless vector-vector decay process B+ ->rho+ rho0. The measurement uses a 78 fb^{-1} data sample collected with the Belle detector at the KEKB asymmetric e+e- collider operating at the Upsilon(4S) resonance. We obtain a branching fraction of Br(B+ ->rho+ rho0)=(31.7+-7.1(stat.)+3.8-6.7(sys.))*10^{-6}. An analysis of the rho helicity-angle distributions gives a longitudinal polarization of Gamma_{L}/Gamma=(94.8+-10.6(stat.)+-2.1(sys.))%.
With advancements in hardware, high-quality HMD devices are being developed by numerous companies, driving increased consumer interest in AR, VR, and MR applications. In this work, we present a new dataset, called VRBiom, of periocular videos acquired using a Virtual Reality headset. The VRBiom, targeted at biometric applications, consists of 900 short videos acquired from 25 individuals recorded in the NIR spectrum. These 10s long videos have been captured using the internal tracking cameras of Meta Quest Pro at 72 FPS. To encompass real-world variations, the dataset includes recordings under three gaze conditions: steady, moving, and partially closed eyes. We have also ensured an equal split of recordings without and with glasses to facilitate the analysis of eye-wear. These videos, characterized by non-frontal views of the eye and relatively low spatial resolutions (400 x 400), can be instrumental in advancing state-of-the-art research across various biometric applications. The VRBiom dataset can be utilized to evaluate, train, or adapt models for biometric use-cases such as iris and/or periocular recognition and associated sub-tasks such as detection and semantic segmentation. In addition to data from real individuals, we have included around 1100 PA constructed from 92 PA instruments. These PAIs fall into six categories constructed through combinations of print attacks (real and synthetic identities), fake 3D eyeballs, plastic eyes, and various types of masks and mannequins. These PA videos, combined with genuine (bona-fide) data, can be utilized to address concerns related to spoofing, which is a significant threat if these devices are to be used for authentication. The VRBiom dataset is publicly available for research purposes related to biometric applications only.
The combination of recent emerging technologies such as network function virtualization (NFV) and network programmability (SDN) gave birth to the novel Network Slicing paradigm. 5G networks consist of multi-tenant infrastructures capable of offering leased network "slices" to new customers (e.g., vertical industries) enabling a new telecom business model: Slice-as-a-Service (SlaaS). However, as the service demand gets increasingly dense, slice requests congestion may occur leading to undesired waiting periods. This may turn into impatient tenant behaviors that increase potential loss of the business attractiveness to customers. In this paper, we aim to i study the slicing admission control problem by means of a multi-queuing system for heterogeneous tenant requests, ii) derive its statistical behavior model, iii) find out the rational strategy of impatient tenants waiting in queue-based slice admission control systems, iv) prove mathematically and empirically the benefits of allowing infrastructure providers to share its information with the upcoming tenants, and v) provide a utility model for network slices admission optimization. Our results analyze the capability of the proposed SlaaS system to be approximately Markovian and evaluate its performance as compared to a baseline solution.
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