Universit`a degli Studi di Genova
Researchers at the University of Toronto, Westlake University, and the University of Electronic Science and Technology of China, along with a global consortium, developed aiXiv, an open-access ecosystem designed for AI-generated scientific content and human-AI collaboration. This platform, featuring a multi-agent review system and iterative refinement, raised the acceptance rate of AI-generated proposals from 0% to 45.2% and papers from 10% to 70% in multi-AI voting, demonstrating enhanced quality and trustworthiness.
Researchers from DIBRIS, Università degli Studi di Genova, extended their Symbolic Pattern Planning (SPP) framework to address temporal numeric planning problems. Their new PATTY_T planner, utilizing a novel SMT encoding, demonstrated superior problem coverage on benchmark domains and consistently found plans with lower abstract step counts than existing symbolic planners.
We present a CloseUpAvatar - a novel approach for articulated human avatar representation dealing with more general camera motions, while preserving rendering quality for close-up views. CloseUpAvatar represents an avatar as a set of textured planes with two sets of learnable textures for low and high-frequency detail. The method automatically switches to high-frequency textures only for cameras positioned close to the avatar's surface and gradually reduces their impact as the camera moves farther away. Such parametrization of the avatar enables CloseUpAvatar to adjust rendering quality based on camera distance ensuring realistic rendering across a wider range of camera orientations than previous approaches. We provide experiments using the ActorsHQ dataset with high-resolution input images. CloseUpAvatar demonstrates both qualitative and quantitative improvements over existing methods in rendering from novel wide range camera positions, while maintaining high FPS by limiting the number of required primitives.
Wide-scale use of visual surveillance in public spaces puts individual privacy at stake while increasing resource consumption (energy, bandwidth, and computation). Neuromorphic vision sensors (event-cameras) have been recently considered a valid solution to the privacy issue because they do not capture detailed RGB visual information of the subjects in the scene. However, recent deep learning architectures have been able to reconstruct images from event cameras with high fidelity, reintroducing a potential threat to privacy for event-based vision applications. In this paper, we aim to anonymize event-streams to protect the identity of human subjects against such image reconstruction attacks. To achieve this, we propose an end-to-end network architecture jointly optimized for the twofold objective of preserving privacy and performing a downstream task such as person ReId. Our network learns to scramble events, enforcing the degradation of images recovered from the privacy attacker. In this work, we also bring to the community the first ever event-based person ReId dataset gathered to evaluate the performance of our approach. We validate our approach with extensive experiments and report results on the synthetic event data simulated from the publicly available SoftBio dataset and our proposed Event-ReId dataset.
Kernel methods provide a powerful framework for non parametric learning. They are based on kernel functions and allow learning in a rich functional space while applying linear statistical learning tools, such as Ridge Regression or Support Vector Machines. However, standard kernel methods suffer from a quadratic time and memory complexity in the number of data points and thus have limited applications in large-scale learning. In this paper, we propose Snacks, a new large-scale solver for Kernel Support Vector Machines. Specifically, Snacks relies on a Nyström approximation of the kernel matrix and an accelerated variant of the stochastic subgradient method. We demonstrate formally through a detailed empirical evaluation, that it competes with other SVM solvers on a variety of benchmark datasets.
Learning embeddings of entities and relations is an efficient and versatile method to perform machine learning on relational data such as knowledge graphs. In this work, we propose holographic embeddings (HolE) to learn compositional vector space representations of entire knowledge graphs. The proposed method is related to holographic models of associative memory in that it employs circular correlation to create compositional representations. By using correlation as the compositional operator HolE can capture rich interactions but simultaneously remains efficient to compute, easy to train, and scalable to very large datasets. In extensive experiments we show that holographic embeddings are able to outperform state-of-the-art methods for link prediction in knowledge graphs and relational learning benchmark datasets.
172
A search for Dark Sectors is performed using the unique M2 beam line at the CERN Super Proton Synchrotron. New particles (XX) could be produced in the bremsstrahlung-like reaction of high energy 160 GeV muons impinging on an active target, μNμNX\mu N\rightarrow\mu NX, followed by their decays, XinvisibleX\rightarrow\text{invisible}. The experimental signature would be a scattered single muon from the target, with about less than half of its initial energy and no activity in the sub-detectors located downstream the interaction point. The full sample of the 2022 run is analyzed through the missing energy/momentum channel, with a total statistics of (1.98±0.02)×1010(1.98\pm0.02)\times10^{10} muons on target. We demonstrate that various muon-philic scenarios involving different types of mediators, such as scalar or vector particles, can be probed simultaneously with such a technique. For the vector-case, besides a LμLτL_\mu-L_\tau ZZ' vector boson, we also consider an invisibly decaying dark photon (AinvisibleA'\rightarrow\text{invisible}). This search is complementary to NA64 running with electrons and positrons, thus, opening the possibility to expand the exploration of the thermal light dark matter parameter space by combining the results obtained with the three beams.
CNRS logoCNRSCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of OsloHeidelberg UniversityUniversity of Waterloo logoUniversity of WaterlooMonash University logoMonash UniversityUniversity of UtahUniversity College London logoUniversity College LondonUniversity of Oxford logoUniversity of OxfordUniversity of California, Irvine logoUniversity of California, IrvineUniversity of Copenhagen logoUniversity of CopenhagenUniversity of EdinburghINFN logoINFNCSICNASA Goddard Space Flight Center logoNASA Goddard Space Flight CenterUniversidade de LisboaCERN logoCERNUniversité Paris-Saclay logoUniversité Paris-SaclayHelsinki Institute of PhysicsUniversity of HelsinkiPerimeter Institute for Theoretical Physics logoPerimeter Institute for Theoretical PhysicsSorbonne Université logoSorbonne UniversitéUniversity of TurkuCEA logoCEAÉcole Polytechnique Fédérale de Lausanne (EPFL)University of BelgradeENS de LyonUniversity of PortsmouthThe Ohio State University logoThe Ohio State UniversityLudwig-Maximilians-Universität MünchenUniv LyonUniversit`a degli Studi di GenovaUniversidade do PortoObservatoire de ParisTechnical University of DenmarkUniversity of TartuCentro de Astrofísica da Universidade do PortoINAF - Osservatorio Astrofisico di TorinoDurham University logoDurham UniversityUniversity of Groningen logoUniversity of GroningenUniversity of BathNiels Bohr InstituteUniversit ́e de Gen`eveJet Propulsion LaboratoryUniversity of NottinghamUniversity of Central LancashireSISSACNESUniversit`a di BolognaPSL Research UniversityUniversidad de La LagunaLaboratoire LagrangeObservatoire de la Côte d’AzurUniversity of Hawai’iUniversit`a degli Studi di MilanoINAF – Istituto di Astrofisica e Planetologia SpazialiKapteyn Astronomical InstituteMax Planck Institute for AstronomyObservatoire astronomique de StrasbourgThe Barcelona Institute of Science and TechnologyUniversity of JyvaskylaLaboratoire d’Astrophysique de MarseilleOzGrav: The ARC Centre of Excellence for Gravitational-Wave DiscoveryINAF – Osservatorio Astronomico di RomaGrenoble-INPInstitut d'Astrophysique de ParisUniversidad de SalamancaInstitut de Física d’Altes Energies (IFAE)Institut d’Estudis Espacials de Catalunya (IEEC)Università della CalabriaLaboratoire de Physique des 2 Infinis Irène Joliot-CurieUniversità degli Studi di Roma "Tor Vergata"INAF-IASF MilanoInstitute of Space ScienceUniversidade de CoimbraLAPThCentro de Investigaciones Energéticas, Medioambientales y Tecnológicas (CIEMAT)European Space Agency (ESA)Tartu ObservatoryInstitució Catalana de Recerca i Estudis Avançats (ICREA)Universit`a Degli Studi Di Napoli “Federico II”Astroparticule et CosmologieUniversidade Federal de Juiz de ForaAIMCPPMDeimos Space S.L.U.LERMAAgenzia Spaziale Italiana (ASI)Museo Storico della Fisica e Centro Studi e Ricerche Enrico FermiInstituto de Física Teórica UAM/CSICIP2I LyonUniv Claude Bernard Lyon 1CFisUCUniversit`a degli Studi di FerraraLaboratoire Univers et Théories LUThObservatoire de SauvernyPort d’Informació CientíficaCentre de Recherche Astrophysique de Lyon (CRAL)Space Research CentreUniversit ́e Cte d’AzurLPSC-Université Grenoble AlpesUniversit`a degli Studi di Milano StataleIATE, CONICET – Universidad Nacional de C ́ordobaUniversitat Politècnica de CartagenaAlma Mater Studiorum · Università di BolognaCosmic Dawn Center(DAWN)Institute of Space Sciences (ICE–CSIC)Universit de ParisUniversidad Autnoma de MadridINAF Osservatorio Astronomico di CapodimonteUniversit degli Studi di PadovaUniversit at BonnUniversit Savoie Mont BlancUniversit Paris CitUniversit de StrasbourgRWTH Aachen UniversityMax Planck-Institute for Extraterrestrial PhysicsRuhr-University-BochumINAF Osservatorio Astrofisico di ArcetriAix-Marseille Universit eINAF Osservatorio Astronomico di PadovaUniversit degli Studi di TorinoINAF Osservatorio di Astrofisica e Scienza dello Spazio di BolognaIFPU Institute for fundamental physics of the UniverseINAF ` Osservatorio Astronomico di Trieste“Sapienza" Università di Roma
The Euclid Collaboration provides a comprehensive forecast of the Euclid mission's ability to constrain parameterized models of modified gravity, employing model-independent approaches such as Phenomenological Modified Gravity (PMG) and Effective Field Theory (EFT) of Dark Energy. The study predicts that Euclid will improve constraints on PMG parameters by an order of magnitude (e.g., σ(Σ_0) ≈ 2.6% for PMG-1) and achieve world-leading precision on EFT parameters (e.g., σ(α_B,0) ≈ 11.6% for EFT-2), highlighting the critical need for improved theoretical modeling of nonlinear scales to fully exploit the mission's data.
Causal learning is the cognitive process of developing the capability of making causal inferences based on available information, often guided by normative principles. This process is prone to errors and biases, such as the illusion of causality, in which people perceive a causal relationship between two variables despite lacking supporting evidence. This cognitive bias has been proposed to underlie many societal problems, including social prejudice, stereotype formation, misinformation, and superstitious thinking. In this research, we investigate whether large language models (LLMs) develop causal illusions, both in real-world and controlled laboratory contexts of causal learning and inference. To this end, we built a dataset of over 2K samples including purely correlational cases, situations with null contingency, and cases where temporal information excludes the possibility of causality by placing the potential effect before the cause. We then prompted the models to make statements or answer causal questions to evaluate their tendencies to infer causation erroneously in these structured settings. Our findings show a strong presence of causal illusion bias in LLMs. Specifically, in open-ended generation tasks involving spurious correlations, the models displayed bias at levels comparable to, or even lower than, those observed in similar studies on human subjects. However, when faced with null-contingency scenarios or temporal cues that negate causal relationships, where it was required to respond on a 0-100 scale, the models exhibited significantly higher bias. These findings suggest that the models have not uniformly, consistently, or reliably internalized the normative principles essential for accurate causal learning.
ETH Zurich logoETH ZurichCNRS logoCNRSCalifornia Institute of Technology logoCalifornia Institute of TechnologyUniversity of OsloUniversity of Cambridge logoUniversity of CambridgeINFN Sezione di NapoliSLAC National Accelerator LaboratoryCarnegie Mellon University logoCarnegie Mellon UniversityUniversity of Manchester logoUniversity of ManchesterUniversity of ZurichUniversity College London logoUniversity College LondonUniversity of California, Irvine logoUniversity of California, IrvineStanford University logoStanford UniversityUniversity of Copenhagen logoUniversity of CopenhagenUniversity of EdinburghNASA Goddard Space Flight Center logoNASA Goddard Space Flight CenterUniversidade de LisboaLancaster UniversityHelsinki Institute of PhysicsUniversity of HelsinkiUppsala UniversityUniversity of TurkuLeiden University logoLeiden UniversityCEA logoCEAUniversit`a degli Studi di PadovaENS de LyonEcole Polytechnique Federale de Lausanne (EPFL)KTH Royal Institute of Technology logoKTH Royal Institute of TechnologyUniversit`a degli Studi di GenovaUniversidade do PortoUniversity of SussexTechnical University of DenmarkINAF - Osservatorio Astrofisico di TorinoDurham University logoDurham UniversityUniversity of Groningen logoUniversity of GroningenNiels Bohr InstituteJet Propulsion LaboratoryInstituto de Astrofísica de CanariasSISSAINFN, Sezione di TorinoJodrell Bank Centre for AstrophysicsIN2P3Institute of Astronomy, University of CambridgeLaboratoire LagrangeUniversity of Hawai’iEuropean Space Astronomy Centre (ESAC)INAF – Istituto di Astrofisica e Planetologia SpazialiKapteyn Astronomical InstituteThe Barcelona Institute of Science and TechnologyLaboratoire d’Astrophysique de MarseilleUniversidad Autonoma de MadridINAF – Osservatorio Astronomico di RomaGrenoble-INPInstitut d'Astrophysique de ParisUniversidad de SalamancaInstitut de Física d’Altes Energies (IFAE)IPACInstitut d’Estudis Espacials de Catalunya (IEEC)INFN - Sezione di PadovaObservatoire de la Cˆote d’AzurINAF-IASF MilanoInstitute of Space ScienceUniversidade de CoimbraINFN-Sezione di GenovaLAPThIRAPDTU SpaceEuropean Space Agency (ESA)INFN-Sezione di BolognaKavli Institute for Particle Astrophysics and CosmologyUniversite de ToulouseUniversit`a degli Studi di TriesteUniversit`a Degli Studi Di Napoli “Federico II”Leiden ObservatoryINFN-BolognaAIMCPPMUniversit\'e C\^ote d'AzurUniversite de LyonUPS-OMPMullard Space Science LaboratoryInstitute for AstronomySpace Science Data Center – ASILPSC-IN2P3Institut de Ciencies de l’Espai (ICE-CSIC)Universit`a degli Studi di FerraraInstitute of Theoretical AstrophysicsCentre de Physique des Particules de MarseilleDARK Cosmology CentreAix-Marseille Universit\'eMcWilliams Center for CosmologyUniversit‘a della CalabriaInstitute for Computational Science, University of ZurichCentre de Recherche Astrophysique de Lyon UMR5574Institut de Physique Nucleaire de LyonCentre National d’Etudes Spatiales (CNES)Universitat InnsbruckUniversidad Politecnica de CartagenaInstituto de Astrofísica e Ciˆencias do Espa̧coUniversit`a degli Studi di Milano StataleUniversit´e Paris Cit´eInstituto de F́ısica Téorica UAM/CSICPort d’Informaci´o Cient´ıfica (PIC)Serco ESA Technical GMBHLaboratoire d’Astrophysique (LASTRO)Universit´e de Grenoble AlpesCentro de F´ısica das Universidades de CoimbraInstitut f¨ur Astro- und TeilchenphysikCentre de Donn´ees astronomiques de StrasbourgUniversit´e Claude Bernard (Lyon 1)Alma Mater Studiorum · Università di BolognaCosmic Dawn Center(DAWN)INAF Osservatorio Astronomico di CapodimonteUniversit at BonnUniversité Paris-SaclayMax Planck-Institute for Extraterrestrial PhysicsINAF Osservatorio Astrofisico di ArcetriLudwig-Maximilians-Universit ¨at M ¨unchenMax Planck Institut fur AstronomieINAF Osservatorio di Astrofisica e Scienza dello Spazio di BolognaArgelander Institut f ür AstronomieIFPU Institute for fundamental physics of the UniverseINFN Sezione di TriesteINAF ` Osservatorio Astronomico di TriesteUniversite de GeneveUniversita' degli Studi di TorinoUniversité Savoie-Mont BlancINAF Osservatorio Astronomico di Brera“Sapienza" Università di RomaSorbonne Université
To date, galaxy image simulations for weak lensing surveys usually approximate the light profiles of all galaxies as a single or double Sérsic profile, neglecting the influence of galaxy substructures and morphologies deviating from such a simplified parametric characterization. While this approximation may be sufficient for previous data sets, the stringent cosmic shear calibration requirements and the high quality of the data in the upcoming Euclid survey demand a consideration of the effects that realistic galaxy substructures have on shear measurement biases. Here we present a novel deep learning-based method to create such simulated galaxies directly from HST data. We first build and validate a convolutional neural network based on the wavelet scattering transform to learn noise-free representations independent of the point-spread function of HST galaxy images that can be injected into simulations of images from Euclid's optical instrument VIS without introducing noise correlations during PSF convolution or shearing. Then, we demonstrate the generation of new galaxy images by sampling from the model randomly and conditionally. Next, we quantify the cosmic shear bias from complex galaxy shapes in Euclid-like simulations by comparing the shear measurement biases between a sample of model objects and their best-fit double-Sérsic counterparts. Using the KSB shape measurement algorithm, we find a multiplicative bias difference between these branches with realistic morphologies and parametric profiles on the order of 6.9×1036.9\times 10^{-3} for a realistic magnitude-Sérsic index distribution. Moreover, we find clear detection bias differences between full image scenes simulated with parametric and realistic galaxies, leading to a bias difference of 4.0×1034.0\times 10^{-3} independent of the shape measurement method. This makes it relevant for stage IV weak lensing surveys such as Euclid.
13 Oct 2010
The aim of this work is to develop a study from the perspective of Abstract Algebraic Logic of some bilattice-based logical systems introduced in the nineties by Ofer Arieli and Arnon Avron. The motivation for such an investigation has two main roots. On the one hand there is an interest in bilattices as an elegant formalism that gave rise in the last two decades to a variety of applications, especially in the field of Theoretical Computer Science and Artificial Intelligence. In this respect, the present study aims to be a contribution to a better understanding of the mathematical and logical framework that underlie these applications. On the other hand, our interest in bilattice-based logics comes from Abstract Algebraic Logic. In very general terms, algebraic logic can be described as the study of the connections between algebra and logic. One of the main reasons that motivate this study is the possibility to treat logical problems with algebraic methods and viceversa: this is accomplished by associating to a logical system a class of algebraic models that can be regarded as the algebraic counterpart of that logic. Starting from the work of Tarski and his collaborators, the method of algebraizing logics has been increasingly developed and generalized. In the last two decades, algebraic logicians have focused their attention on the process of algebraization itself: this kind of investigation forms now a subfield of algebraic logic known as Abstract Algebraic Logic (which we abbreviate AAL).
The inclusion of an additional U(1)U(1) gauge LμLτL_\mu-L_\tau symmetry would release the tension between the measured and the predicted value of the anomalous muon magnetic moment: this paradigm assumes the existence of a new, light ZZ^\prime vector boson, with dominant coupling to μ\mu and τ\tau leptons and interacting with electrons via a loop mechanism. The LμLτL_\mu-L_\tau model can also explain the Dark Matter relic abundance, by assuming that the ZZ' boson acts as a "portal" to a new Dark Sector of particles in Nature, not charged under known interactions. In this work we present the results of the ZZ' search performed by the NA64-ee experiment at CERN SPS, that collected 9×1011\sim 9\times10^{11} 100 GeV electrons impinging on an active thick target. Despite the suppressed ZZ' production yield with an electron beam, NA64-ee provides the first accelerator-based results excluding the g2g-2 preferred band of the ZZ' parameter space in the 1 keV < m_{Z'} \lesssim 2 MeV range, in complementarity with the limits recently obtained by the NA64-μ\mu experiment with a muon beam.
This paper proposes a data-driven approach for constructing firmly nonexpansive operators. We demonstrate its applicability in Plug-and-Play (PnP) methods, where classical algorithms such as Forward-Backward splitting, Chambolle-Pock primal-dual iteration, Douglas-Rachford iteration or alternating directions method of multipliers (ADMM), are modified by replacing one proximal map by a learned firmly nonexpansive operator. We provide sound mathematical background to the problem of learning such an operator via expected and empirical risk minimization. We prove that, as the number of training points increases, the empirical risk minimization problem converges (in the sense of Gamma-convergence) to the expected risk minimization problem. Further, we derive a solution strategy that ensures firmly nonexpansive and piecewise affine operators within the convex envelope of the training set. We show that this operator converges to the best empirical solution as the number of points in the envelope increases in an appropriate way. Finally, the experimental section details practical implementations of the method and presents an application in image denoising, where we consider a novel, interpretable PnP Chambolle-Pock primal-dual iteration.
Institute for Computational and Data SciencesCNRS logoCNRSAcademia SinicaUniversity of Cambridge logoUniversity of CambridgeMonash University logoMonash UniversityNational Central UniversityUniversita di PisaUniversity of Chicago logoUniversity of ChicagoNikhefGeorgia Institute of Technology logoGeorgia Institute of Technologythe University of Tokyo logothe University of TokyoPusan National UniversityStanford University logoStanford UniversityUniversity of Bristol logoUniversity of BristolUniversity of Copenhagen logoUniversity of CopenhagenThe Chinese University of Hong Kong logoThe Chinese University of Hong KongUniversity of MelbourneINFN logoINFNUniversity of WarsawUniversita di PerugiaNASA Goddard Space Flight Center logoNASA Goddard Space Flight CenterLouisiana State UniversityInternational Centre for Theoretical Sciences, Tata Institute of Fundamental ResearchUniversit‘a di Napoli Federico IIUniversity of Florida logoUniversity of FloridaUniversity of Minnesota logoUniversity of MinnesotaUniversity of Maryland logoUniversity of MarylandSeoul National University logoSeoul National UniversityNational Taiwan Normal UniversityThe Pennsylvania State University logoThe Pennsylvania State UniversityRochester Institute of TechnologyChennai Mathematical InstituteKing’s College London logoKing’s College LondonIndian Institute of Technology, BombayScuola Superiore MeridionaleNational Changhua University of EducationCharles Sturt UniversityAustralian National University logoAustralian National UniversityUniversity of Western AustraliaUniversity of GlasgowHigh Energy Accelerator Research Organization (KEK)The Graduate University for Advanced Studies (SOKENDAI)Universit`a degli Studi di GenovaWigner Research Centre for PhysicsUniversity of Alabama in HuntsvilleSyracuse UniversityNicolaus Copernicus Astronomical Center, Polish Academy of SciencesObservatoire de ParisInstituto Nacional de Pesquisas EspaciaisIndian Institute of Technology DelhiUniversitat de les Illes BalearsLomonosov Moscow State UniversitySouthwest Jiaotong UniversityUniversity of BirminghamNational Cheng Kung UniversityColl`ege de FranceNiels Bohr InstituteWashington State UniversityINFN, Laboratori Nazionali del Gran SassoGran Sasso Science Institute (GSSI)University of OregonCalifornia State University, FullertonNational Tsing-Hua UniversityBar Ilan UniversityUniversity of AdelaideUniversite Libre de BruxellesIndian Institute of Technology GandhinagarUniversit`a di BolognaMax Planck Institute for Gravitational Physics (Albert Einstein Institute)Universite catholique de LouvainUniversitat de ValenciaResonac CorporationInstitute for Plasma ResearchInter-University Centre for Astronomy and AstrophysicsWest Virginia UniversityCNR-SPINInstituto de Astrofísica de AndalucíaObservatoire de la Cˆote d’AzurIJCLabLaboratoire Kastler BrosselUniversity of ToyamaUniversit`a di Roma TreLaboratoire Charles CoulombUniversity of SzegedUniversity of Wisconsin–MilwaukeeNational Synchrotron Radiation Research CenterKorea Institute of Science and Technology InformationUniversite de StrasbourgLIGO Hanford ObservatoryUniversit‘a di SalernoLIGO, California Institute of TechnologyUniversit\'e C\^ote d'AzurLUTHThe University of Texas Rio Grande ValleyNational Astronomical Observatory of Japan (NAOJ)National Institute for Mathematical SciencesLIGO Livingston ObservatoryIP2I LyonLeibniz Universit\"at HannoverUniversit´e de MontpellierUniversit\`a degli Studi di Urbino ‘Carlo Bo’Laboratoire de l'Accelerateur LineaireUniversit`e de Li`egeLaboratoire de Physique des 2 Infinis Ir`ene Joliot-CurieInstitut FOTONUniversit`a degli Studi di UdineEuropean Gravitational Observatory (EGO)Inje UniversityUniversite du Littoral - Cote d’OpaleLaboratoire d’Annecy de Physique des Particules (LAPP)Universit`a della Campania “Luigi Vanvitelli”Universit´e Paris Cit´eIPHC UMR 7178Key Laboratory of Quantum Optics and Quantum InformationUniversit`a di Cassino e del Lazio MeridionaleUniversit`a degli Studi di SannioCentre Scientifique et Technique du BˆatimentDirectorate of Knowledge Management in Healthcare, Sree Chitra Tirunal Institute for Medical Sciences and TechnologyInstitute for Astronomical ScienceUniversit´e Claude Bernard (Lyon 1)Friedrich-Schiller-Universität JenaÉ́cole normale supérieureUniversita di ParmaUniversité Paris-SaclayUniversită di CagliariUniversità degli Studi di Napoli “Parthenope”Universita' di SienaUniv-RennesINAF Osservatorio Astronomico di PadovaUniversita di Roma ‘La Sapienza’Universita' di PadovaUniversité PSLSorbonne Université
We search for gravitational-wave signals associated with gamma-ray bursts detected by the Fermi and Swift satellites during the second half of the third observing run of Advanced LIGO and Advanced Virgo (1 November 2019 15:00 UTC-27 March 2020 17:00 UTC).We conduct two independent searches: a generic gravitational-wave transients search to analyze 86 gamma-ray bursts and an analysis to target binary mergers with at least one neutron star as short gamma-ray burst progenitors for 17 events. We find no significant evidence for gravitational-wave signals associated with any of these gamma-ray bursts. A weighted binomial test of the combined results finds no evidence for sub-threshold gravitational wave signals associated with this GRB ensemble either. We use several source types and signal morphologies during the searches, resulting in lower bounds on the estimated distance to each gamma-ray burst. Finally, we constrain the population of low luminosity short gamma-ray bursts using results from the first to the third observing runs of Advanced LIGO and Advanced Virgo. The resulting population is in accordance with the local binary neutron star merger rate.
A cyber range is an environment used for training security experts and testing attack and defence tools and procedures. Usually, a cyber range simulates one or more critical infrastructures that attacking (red) and defending (blue) teams must compromise and protect, respectively. The infrastructure can be physically assembled, but much more convenient is to rely on the Infrastructure as a Service (IaaS) paradigm. Although some modern technologies support the IaaS, the design and deployment of scenarios of interest is mostly a manual operation. As a consequence, it is a common practice to have a cyber range hosting few (sometimes only one), consolidated scenarios. However, reusing the same scenario may significantly reduce the effectiveness of the training and testing sessions. In this paper, we propose a framework for automating the definition and deployment of arbitrarily complex cyber range scenarios. The framework relies on the virtual scenario description language (VSDL), i.e., a domain-specific language for defining high-level features of the desired infrastructure while hiding low-level details. The semantics of VSDL is given in terms of constraints that must be satisfied by the virtual infrastructure. These constraints are then submitted to an SMT solver for checking the satisfiability of the specification. If satisfiable, the specification gives rise to a model that is automatically converted to a set of deployment scripts to be submitted to the IaaS provider.
Many of the blazars observed by Fermi actually have the peak of their time-averaged gamma-ray emission outside the \sim GeV Fermi energy range, at \sim MeV energies. The detailed shape of the emission spectrum around the \sim MeV peak places important constraints on acceleration and radiation mechanisms in the blazar jet and may not be the simple broken power law obtained by extrapolating from the observed X-ray and GeV gamma-ray spectra. In particular, state-of-the-art simulations of particle acceleration by shocks show that a significant fraction (possibly up to 90%\approx 90\%) of the available energy may go into bulk, quasi-thermal heating of the plasma crossing the shock rather than producing a non-thermal power law tail. Other ``gentler" but possibly more pervasive acceleration mechanisms such as shear acceleration at the jet boundary may result in a further build-up of the low-energy ($\gamma \lesssim 10^{2}$) electron/positron population in the jet. As already discussed for the case of gamma-ray bursts, the presence of a low-energy, Maxwellian-like ``bump'' in the jet particle energy distribution can strongly affect the spectrum of the emitted radiation, e.g., producing an excess over the emission expected from a power-law extrapolation of a blazar's GeV-TeV spectrum. We explore the potential detectability of the spectral component ascribable to a hot, quasi-thermal population of electrons in the high-energy emission of flat-spectrum radio quasars (FSRQ). We show that for typical FSRQ physical parameters, the expected spectral signature is located at \sim MeV energies. For the brightest Fermi FSRQ sources, the presence of such a component will be constrained by the upcoming MeV Compton Spectrometer and Imager (COSI) satellite.
In this paper, we investigate how to learn rich and robust feature representations for audio classification from visual data and acoustic images, a novel audio data modality. Former models learn audio representations from raw signals or spectral data acquired by a single microphone, with remarkable results in classification and retrieval. However, such representations are not so robust towards variable environmental sound conditions. We tackle this drawback by exploiting a new multimodal labeled action recognition dataset acquired by a hybrid audio-visual sensor that provides RGB video, raw audio signals, and spatialized acoustic data, also known as acoustic images, where the visual and acoustic images are aligned in space and synchronized in time. Using this richer information, we train audio deep learning models in a teacher-student fashion. In particular, we distill knowledge into audio networks from both visual and acoustic image teachers. Our experiments suggest that the learned representations are more powerful and have better generalization capabilities than the features learned from models trained using just single-microphone audio data.
21
The TOTEM experiment at the LHC has performed the first measurement at s=13\sqrt{s} = 13 TeV of the ρ\rho parameter, the real to imaginary ratio of the nuclear elastic scattering amplitude at t=0t=0, obtaining the following results: ρ=0.09±0.01\rho = 0.09 \pm 0.01 and ρ=0.10±0.01\rho = 0.10 \pm 0.01, depending on different physics assumptions and mathematical modelling. The unprecedented precision of the ρ\rho measurement, combined with the TOTEM total cross-section measurements in an energy range larger than 10 TeV (from 2.76 to 13 TeV), has implied the exclusion of all the models classified and published by COMPETE. The ρ\rho results obtained by TOTEM are compatible with the predictions, from alternative theoretical models both in the Regge-like framework and in the QCD framework, of a colourless 3-gluon bound state exchange in the tt-channel of the proton-proton elastic scattering. On the contrary, if shown that the 3-gluon bound state tt-channel exchange is not of importance for the description of elastic scattering, the ρ\rho value determined by TOTEM would represent a first evidence of a slowing down of the total cross-section growth at higher energies. The very low-t|t| reach allowed also to determine the absolute normalisation using the Coulomb amplitude for the first time at the LHC and obtain a new total proton-proton cross-section measurement σtot=110.3±3.5\sigma_{tot} = 110.3 \pm 3.5 mb, completely independent from the previous TOTEM determination. Combining the two TOTEM results yields σtot=110.5±2.4\sigma_{tot} = 110.5 \pm 2.4 mb.
We analyze the learning properties of the stochastic gradient method when multiple passes over the data and mini-batches are allowed. We study how regularization properties are controlled by the step-size, the number of passes and the mini-batch size. In particular, we consider the square loss and show that for a universal step-size choice, the number of passes acts as a regularization parameter, and optimal finite sample bounds can be achieved by early-stopping. Moreover, we show that larger step-sizes are allowed when considering mini-batches. Our analysis is based on a unifying approach, encompassing both batch and stochastic gradient methods as special cases. As a byproduct, we derive optimal convergence results for batch gradient methods (even in the non-attainable cases).
Proton-proton elastic scattering has been measured by the TOTEM experiment at the CERN Large Hadron Collider at {\surd}s = 7 TeV in dedicated runs with the Roman Pot detectors placed as close as seven times the transverse beam size (sbeam) from the outgoing beams. After careful study of the accelerator optics and the detector alignment, |t|, the square of four-momentum transferred in the elastic scattering process, has been determined with an uncertainty of d t = 0.1GeV p|t|. In this letter, first results of the differential cross section are presented covering a |t|-range from 0.36 to 2.5GeV2. The differential cross-section in the range 0.36 < |t| < 0.47 GeV2 is described by an exponential with a slope parameter B = (23.6{\pm}0.5stat {\pm}0.4syst)GeV-2, followed by a significant diffractive minimum at |t| = (0.53{\pm}0.01stat{\pm}0.01syst)GeV2. For |t|-values larger than ~ 1.5GeV2, the cross-section exhibits a power law behaviour with an exponent of -7.8_\pm} 0.3stat{\pm}0.1syst. When compared to predictions based on the different available models, the data show a strong discriminative power despite the small t-range covered.
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