Diego SANCHEZ

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2025
• Auteurs : C BellhouseJ.B Golden-MarxS.P BamfordN.A HatchM KlugeA EllienS.L AhadP DimauroF. DurretA.H GonzalezY Jimenez-TejaM MontesM SerenoE SlezakM BolzonellaG CastignaniO CucciatiG de LuciaZ GhaffariL MoscardiniR PelloL PozzettiTeymoor SaifollahiA.S BorlaffNabila AghanimB AltieriA AmaraS AndreonC BaccigalupiM BaldiS BardelliA BassetP BattagliaR BenderD BoninoE BranchiniM BresciaA CaillatS CameraV CapobiancoC CarboneV.F CardoneJ CarreteroS CasasM CastellanoS CavuotiA CimattiC Colodro-CondeG CongedoC.J ConseliceL ConversiY CopinF CourbinH.M CourtoisJean-Charles CuillandreA da SilvaH DegaudenziA.M Di GiorgioJ DinisF DubathC.A.J DuncanX DupacS DusiniM FarinaS FarrensF FaustiniS FerriolS FotopoulouM FrailisE FranceschiM FumanaS GaleottaK GeorgeB GillisC GiocoliP Gómez-AlvarezA GrazianF GruppS.V.H HauganH HoekstraM.S HollimanW HolmesI HookF HormuthA HornstrupP HudelotK JahnkeM JhabvalaE KeihänenS KermicheA KiesslingM KilbingerB KubikM KümmelM KunzH Kurki-SuonioP LiebingS LigoriP.B LiljeV LindholmI LloroG MainettiD MainoE MaioranoO MansuttiO MarggrafK MarkovicM MartinelliN MartinetF MarulliR MasseyS MaurogordatoE MedinaceliS MeiM MelchiorM MeneghettiE MerlinG MeylanM MorescoR NakajimaC NeissnerS.-M NiemiC PadillaS PaltaniF PasianK PedersenV PettorinoS PiresG PolentaM PoncetL.A PopaF RaisonA RenziJ RhodesG RiccioE RomelliM RoncarelliE RossettiR SagliaZ SakrD SaponeB SartorisP SchneiderT SchrabbackG SeidelS SerranoC SirignanoG SirriL StancoJ SteinwagnerP Tallada-CrespíI TerenoR Toledo-MoreoF TorradeflotA TsyganovI TutusausL ValenzianoT VassalloG. Verdoes KleijnA VeropalumboY WangJ WellerG ZamoraniElena ZuccaA BivianoE BozzoC BuriganaM CalabreseD Di FerdinandoJ.A. Escartin VigoR FarinelliF FinelliL GabarraJ Gracia-CarpioS MatthewN MauriA MoraM PöntinenV ScottezP SimonM TentiM VielM WiesmannY AkramiI.T AndikaS AnselmiM ArchidiaconoF Atrio-BarandelaM BallardiniMatthieu BétherminA BlanchardL BlotH BöhringerS BorganiM.L BrownS BrutonRémi CabanacA CalabroG Cañas-HerreraA CappiF CaroC.S CarvalhoT CastroK.C ChambersF CogatoT. ContiniA.R CoorayF de PaolisG DesprezA Díaz-SánchezJ.J DiazS Di DomizioJ.M DiegoH DoleStephanie EscoffierA.G FerrariP.G FerreiraA FinoguenovA FontanaK GangaJ García-BellidoT GasparettoE GaztanagaF GiacominiF GianottiG GozaliaslA GregorioM GuidiC.M GutierrezA HallW.G HartleyS HemmatiH HildebrandtJ HjorthA. Jimenez MuñozJ.J.E KajavaY KangV KansalD KaragiannisC.C KirkpatrickS KrukM LattanziA.M.C Le BrunJ Le GraetL LegrandM LemboJ LesgourguesT.I LiaudatS.J LiuA LoureiroM MagliocchettiF MannucciR MaoliJ Martín-FleitasC.J.A.P MartinsL MaurinR.B MetcalfM MiluzioP MonacoC MorettiG MorganteC MurrayK NaidooA Navarro-AlsinaS NesserisK PatersonL PatriziiA PisaniV PopaD PotterI RissoP.-F RocciM SahlénE SarpaA SchneiderM SchultheisD SciottiE SellentinL.C SmithS.A StanfordK TanidisC TaoG TesteraR TeyssierS ToftS TosiA TrojaM TucciC ValieriJussi ValiviitaD VerganiG VerzaP VielzeufN.A Walton
• Organismes : Joseph Louis LAGRANGE Institut d'Astrophysique de Paris Joseph Louis LAGRANGE Laboratoire d'Astrophysique de Marseille Observatoire astronomique de Strasbourg Institut d'astrophysique spatiale Centre National d'Études Spatiales [Toulouse] Laboratoire d'Astrophysique de Marseille Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Astrophysique Interprétation Modélisation Astrophysique Interprétation Modélisation Institut de Physique des 2 Infinis de Lyon Institut d'Astrophysique de Paris Centre de Physique des Particules de Marseille Astrophysique Interprétation Modélisation Institut de Physique des 2 Infinis de Lyon Centre de Calcul de l'IN2P3 Laboratoire d'Astrophysique de Marseille Joseph Louis LAGRANGE AstroParticule et Cosmologie Agence Spatiale Européenne = European Space Agency Agence Spatiale Européenne = European Space Agency Astrophysique Interprétation Modélisation Centre National d'Études Spatiales [Toulouse] Institut de recherche en astrophysique et planétologie Institut de recherche en astrophysique et planétologie Institut d'Astrophysique de Paris Université de Lille, Sciences et Technologies Laboratoire Univers et Théories Observatoire astronomique de Strasbourg Institut de recherche en astrophysique et planétologie Laboratoire Univers et Théories Institut de recherche en astrophysique et planétologie Agence Spatiale Européenne = European Space Agency Joseph Louis LAGRANGE Institut de recherche en astrophysique et planétologie Institut d'astrophysique spatiale Centre de Physique des Particules de Marseille AstroParticule et Cosmologie Laboratoire de Physique Subatomique et de Cosmologie Laboratoire Univers et Théories Centre de Physique des Particules de Marseille Institut de Recherches sur les lois Fondamentales de l'Univers Institut d'astrophysique spatiale AstroParticule et Cosmologie Centre de Physique des Particules de Marseille Institut d'astrophysique spatiale Joseph Louis LAGRANGE Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille
• Publié dans Astron.Astrophys. le 02/11/2025

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Résumé : 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 ($10^{13.9}$-$10^{15.0}$ 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 $10^{14.2}$ 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 $\sim80000$ clusters of $>10^{14.2}$ M$_\odot$ between $z=0.3$ and 1.5 with a S/N$>3$. Half of these clusters will reside below $z=0.75$ and the majority of those below $z=0.6$ will be detected with a S/N $>20$. A few thousand clusters at $1.310^{14.7}$ M$_\odot$. Euclid will detect the ICL at more than 500 kpc distance from the BCG, up to $z=0.7$, in several hundred of these massive clusters over its large survey volume.

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Fichiers liés : aa53887-25.pdf

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2025
• Auteurs : Aram HayrapetyanArmen TumasyanWolfgang AdamJanik Walter AndrejkovicThomas BergauerSuman ChatterjeeKonstantinos DamanakisMarko DragicevicPriya Sajid HussainManfred JeitlerNatascha KrammerAng LiDietrich LikoIvan MikulecJochen SchieckRobert SchöfbeckDennis SchwarzMangesh SonawaneSebastian TemplWolfgang WaltenbergerClaudia-Elisabeth WulzMohamed Rashad DarwishTahys JanssenPierre van MechelenEmil Sørensen BolsJorgen d'HondtSoumya DansanaAlexandre de MoorMartin DelcourtHesham El FahamSteven LowetteInna MakarenkoDenise MüllerStefaan TavernierMichael TytgatGerrit Patrick van OnsemSenne van PutteDavid VanneromBarbara ClerbauxAloke Kumar DasGilles de LentdeckerHugues EvardLaurent FavartParaskevas GianneiosDmytro HohovJohny JaramilloAli KhalilzadehFakhri Alam KhanKyeongpil LeeMostafa MahdavikhorramiAndrea MalaraSantiago ParedesLaurent ThomasMax Vanden BemdenCatherine Vander VeldePascal VanlaerMaarten de CoenDidar DoburYanwen HongJoscha KnolleLuka LambrechtGianny MestdachKevin Mota AmariloCésar RendónAmrutha SamalanKirill SkovpenNiels van den BosscheJan van der LindenLiam WezenbeekAnna BeneckeAgni BethaniGiacomo BrunoClaudio CaputoChristophe DelaereIzzeddin Suat DonertasAndrea GiammancoSandhya JainVincent LemaitreJindrich LidrychPaola MastrapasquaKuntal MondalTu Thong TranSébastien WertzGilvan AlvesEduardo CoelhoCarsten HenselThales Menezes de OliveiraArthur MoraesPatricia Rebello TelesMariana SoeiroWalter Luiz Aldá JúniorMiguel Alves Gallo PereiraMapse Barroso Ferreira FilhoHelena Brandao MalbouissonWagner CarvalhoJose ChinellatoEliza Melo da CostaGustavo Gil da SilveiraDilson de Jesus DamiaoSandro Fonseca de SouzaRaphael Gomes de SouzaJordan MartinsClemencia Mora HerreraLuiz MundimHelio NogimaJoao Pedro PinheiroAlberto SantoroAndre SznajderMauricio ThielAntonio Vilela PereiraCesar Augusto BernardesLuigi CalligarisThiago TomeiEduardo de Moraes GregoresPedro G MercadanteSergio F NovaesBreno OrzariSandra PadulaAleksandar AleksandrovGeorgy AntchevRoumyana 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• Publié dans Nature Commun. le 25/11/2025

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Résumé : Despite the f$_0$(980) hadron having been discovered half a century ago, the question about its quark content has not been settled: it might be an ordinary quark-antiquark ($\mathrm{q\bar{q}}$) meson, a tetraquark ($\mathrm{q\bar{q}q\bar{q}}$) exotic state, a kaon-antikaon ($\mathrm{K\bar{K}}$) molecule, or a quark-antiquark-gluon ($\mathrm{q\bar{q}g}$) hybrid. This paper reports strong evidence that the f$_0$(980) state is an ordinary $\mathrm{q\bar{q}}$ meson, inferred from the scaling of elliptic anisotropies ($v_2$) with the number of constituent quarks ($n_\mathrm{q}$), as empirically established using conventional hadrons in relativistic heavy ion collisions. The f$_0$(980) state is reconstructed via its dominant decay channel f$_0$(980) $\to$$\pi^+\pi^-$, in proton-lead collisions recorded by the CMS experiment at the LHC, and its $v_2$ is measured as a function of transverse momentum ($p_\mathrm{T}$). It is found that the $n_q$ = 2 ($\mathrm{q\bar{q}}$ state) hypothesis is favored over $n_q$ = 4 ($\mathrm{q\bar{q}q\bar{q}}$ or $\mathrm{K\bar{K}}$ states) by 7.7, 6.3, or 3.1 standard deviations in the $p_\mathrm{T}$$\lt$ 10, 8, or 6 GeV/$c$ ranges, respectively, and over $n_\mathrm{q}$ = 3 ($\mathrm{q\bar{q}g}$ hybrid state) by 3.5 standard deviations in the $p_\mathrm{T}$$\lt$ 8 GeV/$c$ range. This result represents the first determination of the quark content of the f$_0$(980) state, made possible by using a novel approach, and paves the way for similar studies of other exotic hadron candidates.

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2025
• Auteurs : Vladimir ChekhovskyAram HayrapetyanVladimir MakarenkoArmen TumasyanWolfgang AdamJanik Walter AndrejkovicLisa BenatoThomas BergauerSuman ChatterjeeKonstantinos DamanakisMarko DragicevicPriya Sajid HussainManfred JeitlerNatascha KrammerAng LiDietrich LikoIvan MikulecJochen SchieckRobert SchöfbeckDennis SchwarzMangesh SonawaneWolfgang WaltenbergerClaudia-Elisabeth WulzTahys JanssenHyejin KwonThomas van LaerPierre van MechelenNordin BreugelmansJorgen d'HondtSoumya DansanaAlexandre de MoorMartin DelcourtFelix HeyenYanwen HongSteven LowetteInna MakarenkoDenise MüllerStefaan TavernierMichael TytgatGerrit Patrick van OnsemSenne van PutteDavid VanneromBugra BilinBarbara ClerbauxAloke Kumar DasIsabelle de BruynGilles de LentdeckerHugues EvardLaurent FavartParaskevas GianneiosAli KhalilzadehFakhri Alam KhanAndrea MalaraMuhammad Aamir ShahzadLaurent ThomasMax Vanden BemdenCatherine Vander VeldePascal VanlaerMaarten de CoenDidar DoburGul GokbulutJoscha KnolleLuka LambrechtDavid MarckxKirill SkovpenNiels van den BosscheJan van der LindenJules VandenbroeckLiam WezenbeekSamuel BeinAnna BeneckeAgni BethaniGiacomo BrunoClaudio CaputoJerome de Favereau de JeneretChristophe DelaereIzzeddin Suat DonertasAndrea GiammancoAhmet Oguz GuzelSandhya JainVincent LemaitreJindrich LidrychPaola MastrapasquaTu Thong TranSemra TurkcaparGilvan AlvesEduardo CoelhoGilson Correia SilvaCarsten HenselThales Menezes de OliveiraClemencia Mora HerreraPatricia Rebello TelesMariana SoeiroEdmilson José Tonelli ManganoteAntonio Vilela PereiraWalter Luiz Aldá JúniorMapse Barroso Ferreira FilhoHelena Brandao MalbouissonWagner CarvalhoJose ChinellatoEliza Melo da CostaGustavo Gil da SilveiraDilson de Jesus DamiaoSandro Fonseca de SouzaRaphael Gomes de SouzaTulio Laux KuhnMatheus MacedoJordan MartinsKevin Mota AmariloLuiz MundimHelio NogimaJoao Pedro PinheiroAlberto SantoroAndre SznajderMauricio ThielCesar Augusto BernardesLuigi CalligarisThiago TomeiEduardo de Moraes GregoresIsabela Maietto 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• Publié dans JHEP le 17/11/2025

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Résumé : This paper presents the first search for the associated production of a Higgs boson with a charm quark (cH), with the Higgs boson decaying to two photons. Associated cH production provides an opportunity to probe the coupling of the Higgs boson to charm quarks. The results are based on a data set of proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS experiment at the LHC, corresponding to an integrated luminosity of 138 fb$^{-1}$. Assuming the standard model (SM) rates for all other Higgs boson production processes, the observed (expected) upper limit at 95% confidence level on the cH signal strength is 243 (355) times the SM prediction. Under the same assumption, the observed (expected) allowed interval on the Higgs boson to charm quark coupling modifier, $\kappa_\mathrm{c}$, is $\lvert \kappa_\mathrm{c} \rvert$ $\lt$ 38.1 ($\lvert \kappa_\mathrm{c} \rvert$ $\lt$ 72.5) at 95% confidence level.

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