Philippe JEAN-PIERRE

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2024
• Auteurs : Shreyasi AcharyaDagmar AdamovaGianluca Aglieri RinellaMichelangelo AgnelloNeelima AgrawalZubayer AhammedShakeel AhmadSang Un AhnIshaan AhujaAlexander AkindinovMohammad Al-TuranyDmitry AleksandrovBruno AlessandroHaidar Masud AlfandaJose Ruben Alfaro MolinaBushra AliAndrea AliciNegin AlizadehvandchaliAnton AlkinJohan AlmeGiacomo AloccoTorsten AltAnna Rita AltamuraIgor AltsybeevMustafa AnaamCristian AndreiNicodemos AndreouAnton AndronicVenelin AnguelovFederico AntinoriPietro AntonioliNicole ApadulaL AphecetcheHarald AppelshaeuserCarolina ArataSilvia ArcelliMauro ArestiRoberta ArnaldiJhoao Gabriel Martins Campos Almeida ArneiroIonut Cristian ArseneMesut ArslandokAndre AugustinusRalf Peter AverbeckMohd Danish AzmiHitoshi BabaAngela BadalaJoonsuk BaeYongwook BaekXiaozhi BaiRaphaelle Marie BailhacheYoshini BailungAlessandro BalbinoAlberto BaldisseriBartosz BalisDebjani BanerjeeZarina BanooRoberto BarberaFrancesco BarileLuca BarioglioMaria BarlouBanajit BarmanGergely Gabor BarnafoldiLee Stuart BarnbyValerie Ramillien BarretLeonardo Barreto de Oliveira CamposClara BartelsKlaus BarthEsther BartschNicole BastidSumit BasuGuillaume BatigneDaniel BattistiniBoris BatyunyaDibakar BauriJose Luis Bazo AlbaIan Gardner BeardenCaitlin BeattiePascal BechtDebadatta BeheraIouri BelikovAilec Bell HechavarriaFrancesca BelliniRene BellwiedSvetlana BelokurovaYael Antonio Vasquez BeltranGyula BencediStefania Maria BeoleYaroslav BerdnikovAnastasia BerdnikovaLuisa BergmannMihaela Gabriela BesoiuLatchezar BetevPartha Pratim BhaduriAnju BhasinMohammad Asif BhatBuddhadeb BhattacharjeeLivio BianchiNicola BianchiJaroslav BielcikJana BielcikovaJacek Bogumil BiernatAlexandre Patrick BigotAnte BilandzicGabor BiroSaikat BiswasNicolas BizéJustin Thomas BlairDmitry BlauMihail Bogdan BlidaruNora BluhmeChristoph BlumeGianluigi BocaFriederike BockTea BodovaAlexey BogdanovStefano BoiJeongsu BokLaszlo BoldizsarMarek BombaraPeter Matthew BondGermano BonomiHerve BorelAlexander BorissovAndres Gerardo Borquez CarcamoHannah BossiElena BottaYoussef El Mard BouzianiLars BratrudPeter Braun-MunzingerMarco BregantMichal BrozGiuseppe Eugenio BrunoMatthew Daniel BucklandDmitry BudnikovHenner BueschingStefania BufalinoPaul Alois BuhlerNazar BurmasovEdith Zinhle ButheleziAleksandr BylinkinSebastian Adam BysiakMengke CaiHelen Louise CainesAlberto CalivaErnesto Calvo VillarJuan Manuel Mejia CamachoPaolo CameriniFabio de Moraes CanedoMihai CarabasAitor Amatriain CarballoFrancesca CarnesecchiRobin Albert Andre CaronLeopoldo Abranches de CarvalhoJavier Ernesto Castillo CastellanosFabio CatalanoCesar Ceballos SanchezIrakli ChakaberiaPritam ChakrabortySinjini ChandraSylvain ChapelandMarielle ChartierSubhasis ChattopadhyaySukalyan ChattopadhyayTonatiuh Garcia ChavezTiantian ChengCvetan Valeriev CheshkovBrigitte CheynisVasco Miguel Chibante BarrosoDavid Dobrigkeit ChinellatoEmma Sophia ChizzaliJaeyoon ChoSoyeon ChoPeter ChochulaDhrubajyoti ChoudhuryPanagiotis ChristakoglouChristian Holm ChristensenPeter ChristiansenTatsuya ChujoMario CiaccoCorrado CicaloFederico CindoloMichael Rudolf CiupekGiulia ClaiFabio Filippo ColamariaJonathan Samuel ColburnDomenico ColellaManuel ColocciMatteo ConcasG. 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• Publié dans JHEP le 14/01/2026

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Résumé : The transverse momentum ($p_{\rm T}$) and centrality dependence of the nuclear modification factor $R_{\rm AA}$ of prompt and non-prompt J$/\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV. The measurements are carried out through the ${\rm e}^{+}{\rm e}^{-}$ decay channel at midrapidity ($|y| < 0.9$) in the transverse momentum region $1.5 < p_{\rm T} < 10$ GeV/$c$. Both prompt and non-prompt J$/\psi$ measurements indicate a significant suppression for $p_{\rm T} >$ 5 GeV/$c$, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_{\rm T}$ intervals, and cover the kinematic region down to $p_{\rm T}$ = 1.5 GeV/$c$ at midrapidity, not accessible by other LHC experiments. The suppression of prompt J$/\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J$/\psi$ production from recombination of c and $\overline{\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J$/\psi$. For non-prompt J$/\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark$-$gluon plasma is consistent with measurements within uncertainties.

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Fichiers liés : JHEP02(2024)066.pdf

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2024
• Auteurs : Adam Abed AbudBabak AbiRoberto AcciarriMario AceroMarcio AdamesGeorge AdamovMark AdamowskiDavid AdamsMarco AdinolfiCris AdrianoAntoni AduszkiewiczJessica AguilarBenjamin AimardFaiza AkbarKyle AllisonSaul Alonso MonsalveMunera AlrashedAndrew AltonRodrigo AlvarezHamza AmarPablo AmedoJohn AndersonDiego Andrade AldanaCostas AndreopoulosMirco AndreottiMichael P AndrewsFenompanirina AndrianalaSofia AndringaNikolay AnfimovArtur AnkowskiMarcelo AntoniassiMaria AntonovaAlexander AntoshkinAlfredo Aranda-FernandezLuciano ArellanoEnrique Arrieta DiazManuel ArroyaveJonathan AsaadiAdi AshkenaziLily AsquithEdward AtkinDidier AugusteAdam AurisanoVladimir AushevDario AutieroFarrukh AzfarAshley BackHenning BackJohn BackIuri BagaturiaLinda BagbyNikita BalashovSupraja BalasubramanianPierre BaldiWander BaldiniBruce BallerBindu BambahRituparna BanerjeeFernando BaraoGabriela BarenboimPablo Barham AlzásGary BarkerWayne BarkhouseGiles BarrJuan Barranco MonarcaAdilson BarrosNuno BarrosDaniel BarrowJoshua BarrowAnastasia Basharina-FreshvilleAmit BashyalVincent BasqueCharlie BatchelorLars Bathe-PetersJames BattatFederico BattistiFatih BayMaria BazettoJosé Luis Bazo AlbaJohn BeacomEdouard BechetoilleBiswaranjan BeheraEwerton BelchiorGerard BellLeo BellantoniGiorgio BellettiniVincenzo BelliniOlga BeltramelloNektarios BenekosCarlos Benitez MontielDouglas BenjaminFrancisco Bento NevesJoshua BergerSophie BerkmanPaolo BernardiniAndrea BersaniSergio BertolucciMinerba BetancourtAmalia Betancur RodríguezAdrian BevanYashwanth BezawadaAnibal BezerraThiago BezerraAvinay BhatVipin BhatnagarJayesh BhattMaharnab BhattacharjeeMeghna BhattacharyaShyam BhullerBipul BhuyanSimone BiagiJianming BianKurt BieryBurak BilkiMary BishaiAlexander BitadzeAndrew BlakeFlor BlaszczykGerald BlazeyEdward BlucherJan BoissevainSara BolognesiTimothy BoltonLuca BombenMaurizio BonesiniCesar Bonilla-DiazFiliberto BoniniAlexander BoothFatma BoranStefania BordoniRafael Borges MerloAran BorkumNilay BostanJuraj BracinikDavide BragaBarnali BrahmaDominic BrailsfordFilippo BramatiAntonio BrancaAndrew BrandtJohan BremerChristopher BrewStephen BriceVanessa BrioClaudia BrizzolariCarl BrombergJim BrookeAlan BrossGiulia BrunettiMaria BrunettiNorman BuchananHoward BuddJonas BuergiDustin BurgardtSophie ButchartGian Caceres VeraIrene CagnoliTejin CaiRoberto CalabreseJacob CalcuttMarius CalinLivio CaliversEnrique CalvoAlessio CaminataWallison CampanelliAxel Campos BenitezNicola CanciJordi CapóIoana CaracasDavid CaratelliDaniel CarberJuan CarcellerGabriella CariniBruno CarlusMateus CarneiroPaolo CarnitiIvan Caro TerrazasHector CarranzaNicholas CarraraLauren CarrollThomas CarrollAlex CarterDenise CasazzaJavier Castaño ForeroF.A CastañoFabian Castaño UsugaAndrés CastilloCesar CastromonteErika Catano-MurCarla CattadoriFabien CavalierFlavio CavannaSandro CentroGiuseppe CeratiAlberto CervelliAnselmo Cervera VillanuevaKaustav ChakrabortyMichel ChalifourAndrew ChappellNikolas CharitonidisAnimesh ChatterjeeHucheng ChenMu-Chun ChenWen Chao ChenYifan ChenZachary Chen-WishartDaniel CherdackCheng-Yi ChiRobert ChircoNamitha ChitirasreemadamKihyeon ChoSarah ChoateDavid ChokheliPooi ChongBarnali ChowdhuryDavid ChristianArtem ChukanovMoses ChungEric ChurchMaria Flavia CicalaMagda CicerchiaValentina CiceroRiccardo CioliniJudicael ClairPeter ClarkeGordon ClineThomas CoanAlfredo CoccoJ.A.B. CoelhoAriel CohenJohann CollotErin ConleyJanet M ConradMark ConveryPeter CookeSimone CopelloPaolo CovaCallum CoxLucien CremaldiLinda CremonesiJosé Crespo-AnadónMichael CrislerEsteban CristaldoJason CrnkovicGordon CroneRyan CrossAndrew CuddClara CuestaYanou CuiDavid CussansJoel DaiOlivia DalagerRicardo DallavalleH da MottaZubair DarRobert DarbyL. da Silva PeresQuentin DavidGavin DaviesStefano DaviniJaime DawsonRenan de AguiarPatricia de AlmeidaPaul DebbinsIsabelle de BonisM.Patrick DecowskiAndre de GouveaPedro de HolandaIker de Icaza AstizPaul de JongAndres de la TorreAlain DelbartDavid DelepineMaritza DelgadoAndrea Dell'AcquaGiovanni Delle MonacheNicola DelmontePatrick de LurgioRoss DemarioJoao de Mello NetoDavid DemuthSteve DennisChris DenshamPeter DentonGrzegorz DeptuchAlbert de RoeckValentina de RomeriJan DetjeJames DevineRanjan DharmapalanMarco DiasJorge S DiazFelix DíazFrancesco Di CapuaAntonio Di DomenicoSergio Di DomizioStefano Di FalcoLetizia Di GiulioPengfei DingLea Di NotoEleonora DiociaiutiCarla DistefanoRichard DiurbaMilind DiwanZelimir DjurcicDionisio DoeringStephen DolanFurkan DolekJ. 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• Organismes : Laboratoire d'Annecy de Physique des Particules Laboratoire de l'Accélérateur Linéaire Institut de Physique des 2 Infinis de Lyon Institut de Physique des 2 Infinis de Lyon Commissariat à l'énergie atomique et aux énergies alternatives Institut de Physique des 2 Infinis de Lyon Laboratoire de l'Accélérateur Linéaire AstroParticule et Cosmologie AstroParticule et Cosmologie Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique Subatomique et de Cosmologie AstroParticule et Cosmologie Institut de Physique des 2 Infinis de Lyon AstroParticule et Cosmologie Laboratoire d'Annecy de Physique des Particules Commissariat à l'énergie atomique et aux énergies alternatives Laboratoire d'Annecy de Physique des Particules Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire Institut de Physique des 2 Infinis de Lyon Laboratoire d'Annecy de Physique des Particules Institut de Physique des 2 Infinis de Lyon AstroParticule et Cosmologie Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire Laboratoire d'Annecy de Physique des Particules Laboratoire de l'Accélérateur Linéaire Laboratoire de Physique Subatomique et de Cosmologie Laboratoire d'Annecy de Physique des Particules Laboratoire d'Annecy de Physique des Particules Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire AstroParticule et Cosmologie Laboratoire de Physique Subatomique et de Cosmologie AstroParticule et Cosmologie Institut de Physique des 2 Infinis de Lyon Laboratoire d'Annecy de Physique des Particules Institut de Physique des 2 Infinis de Lyon Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire AstroParticule et Cosmologie Institut de Physique des 2 Infinis de Lyon Laboratoire de l'Accélérateur Linéaire AstroParticule et Cosmologie Laboratoire de l'Accélérateur Linéaire AstroParticule et Cosmologie AstroParticule et Cosmologie Laboratoire d'Annecy de Physique des Particules
• Publié dans JINST le 08/11/2025

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Résumé : DUNE is an international experiment dedicated to addressing some of the questions at the forefront of particle physics and astrophysics, including the mystifying preponderance of matter over antimatter in the early universe. The dual-site experiment will employ an intense neutrino beam focused on a near and a far detector as it aims to determine the neutrino mass hierarchy and to make high-precision measurements of the PMNS matrix parameters, including the CP-violating phase. It will also stand ready to observe supernova neutrino bursts, and seeks to observe nucleon decay as a signature of a grand unified theory underlying the standard model. The DUNE far detector implements liquid argon time-projection chamber (LArTPC) technology, and combines the many tens-of-kiloton fiducial mass necessary for rare event searches with the sub-centimeter spatial resolution required to image those events with high precision. The addition of a photon detection system enhances physics capabilities for all DUNE physics drivers and opens prospects for further physics explorations. Given its size, the far detector will be implemented as a set of modules, with LArTPC designs that differ from one another as newer technologies arise. In the vertical drift LArTPC design, a horizontal cathode bisects the detector, creating two stacked drift volumes in which ionization charges drift towards anodes at either the top or bottom. The anodes are composed of perforated PCB layers with conductive strips, enabling reconstruction in 3D. Light-trap-style photon detection modules are placed both on the cryostat's side walls and on the central cathode where they are optically powered. This Technical Design Report describes in detail the technical implementations of each subsystem of this LArTPC that, together with the other far detector modules and the near detector, will enable DUNE to achieve its physics goals.

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2024
• Auteurs : Aram HayrapetyanArmen TumasyanWolfgang AdamJanik Walter AndrejkovicThomas BergauerSuman ChatterjeeKonstantinos DamanakisMarko DragicevicAlberto Escalante del VallePriya Sajid HussainManfred JeitlerNatascha KrammerDietrich 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 MüllerAbanti Ranadhir SahasransuStefaan TavernierMichael TytgatSenne van PutteDavid VanneromBarbara ClerbauxGilles de LentdeckerLaurent FavartDmytro HohovJohny JaramilloAli KhalilzadehKyeongpil LeeMostafa MahdavikhorramiAndrea MalaraSantiago ParedesLaurent PétréNicolas PostiauLaurent ThomasMax Vanden BemdenCatherine Vander VeldePascal VanlaerMaarten de CoenDidar DoburYanwen HongJoscha KnolleLuka LambrechtGianny MestdachCésar RendónAmrutha SamalanKirill SkovpenNiels van den BosscheLiam WezenbeekAnna BeneckeGiacomo BrunoClaudio CaputoChristophe DelaereIzzeddin Suat DonertasAndrea GiammancoKhawla JaffelSandhya 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 SouzaJordan MartinsClemencia Mora HerreraKevin Mota AmariloLuiz MundimHelio NogimaAlberto SantoroSheila Mara Silva Do AmaralAndre SznajderMauricio ThielAntonio Vilela PereiraCesar Augusto BernardesLuigi CalligarisThiago TomeiEduardo de Moraes GregoresPedro G MercadanteSergio F NovaesBreno OrzariSandra PadulaAleksandar AleksandrovGeorgy AntchevRoumyana HadjiiskaPlamen IaydjievMilena MishevaMariana ShopovaGeorgi SultanovAnton DimitrovTodor IvanovLeander LitovBorislav PavlovPeicho PetkovAnton PetrovElton ShumkaSumit KeshriShalini ThakurTongguang ChengQianying GuoTahir JavaidMonika MittalLi YuanGerry BauerZhen HuJinfeng LiuKai YiGuo-Ming ChenHe-Sheng ChenMingshui ChenFabio IemmiChun-Hua JiangAnshul KapoorHongbo LiaoZhenan LiuFabio MontiMuhammad Aamir ShahzadRamkrishna SharmaJia-Ning SongJunquan TaoChu WangJin WangZebing WangHuaqiao ZhangAntonis AgapitosYong BanAndrew LevinCongqiao LiQiang LiYajun MaoSi-Jin QianXiaohu SunDayong WangHeng YangLicheng ZhangChen ZhouZhengyun YouNan LuXuyang GaoDuncan LeggatHideki OkawaYu ZhangZhen LinChenfeng LuMeng XiaoCarlos AvilaDiego Andres Barbosa TrujilloAndrés CabreraCarlos FlorezJorge FragaJose Antonio Reyes VegaJhovanny Mejia GuisaoFelipe RamirezManuel RodriguezJosé David Ruiz AlvarezDuje GiljanovicNikola GodinovicDamir LelasAna SculacMarko KovacToni SculacPedrame BargassaVuko BrigljevicBhakti Kanulal ChitrodaDinko FerencekSaswat MishraAndrei 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• Publié dans Phys.Rev.Lett. le 31/10/2025

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Résumé : The first search for scalar leptoquarks produced in lepton-quark collisions and coupled to $\tau$ leptons is presented. It is based on a set of proton-proton collision data recorded with the CMS detector at the LHC at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 138 fb$^{-1}$. The reconstructed final state consists of a jet, significant missing transverse momentum, and a $\tau$ lepton reconstructed through its hadronic or leptonic decays. Limits are set on the product of the leptoquark production cross section and branching fraction and interpreted as exclusions in the plane of the leptoquark mass and the leptoquark-$\tau$-quark coupling strength.

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