Philippe JEAN-PIERRE

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2025
• Auteurs : Georges AadErlend AakvaagBraden Keim AbbottSara AbdelhameedKira AbelingNils Julius AbichtHaider AbidiMohammed AboelelaAsmaa AboulhormaHalina AbramowiczYiming AbulaitiBobby Samir AcharyaAnke AckermannClaire Adam BourdariosLeszek AdamczykSagar AddepalliMatthew John AddisonJahred AdelmanAytul AdiguzelTim AdyeTony AffolderYoav AfikMerve Nazlim AgarasAnamika AggarwalCatalin AgheorghieseiFaig AhmadovSudha AhujaXiaocong AiGiulio AielliArya AikotMalak Ait TamlihatBrahim AitbenchikhMelike AkbiyikTorsten AkessonAndrei AkimovDaiya AkiyamaNilima Nilesh AkolkarSina AktasGian Luigi AlberghiJustin AlbertUna Helena AlbertiPietro AlbicoccoGuillaume Lucas AlbouySara AlderweireldtZackary Lee AlegriaMartin AleksaIgor AlexandrovCalin AlexaTheodoros AlexopoulosFabrizio AlfonsiMalte AlgrenMuhammad AlhroobBabar AliHanadi AliShahzad AliSamuel William AlibocusMalik AlievGianluca AlimontiWael AlkakhiCorentin AllaireBenedict AllbrookeJonny AllenJulia Frances AllenPhilip Patrick AllportAlberto AloisioFrancisco AlonsoCristiano AlpigianiZainab Mohammad K AlsolamiAdrian Alvarez FernandezMario Alves CardosoMariagrazia AlviggiMohamed AlyYara Do Amaral CoutinhoAlessandro AmblerChristoph AmelungMaximilian AmerlChristoph AmesThiziri AmezzaDante AmideiBaktash AminiKyle AmirieArtem AmirkhanovSusana Patricia Amor dos SantosKieran Robert AmosDimitra AmperiadouShiwen AnChristos AnastopoulosTim AndeenJohn Kenneth AndersAdam Campbell AndersonAttilio AndreazzaStylianos AngelidakisAaron AngeramiAlexey AnisenkovAlberto AnnoviClaire AntelEgor AntipovMario AntonelliFabio AnulliMasato AokiTakumi AokiMarco AparoLudovica Aperio BellaMariano ApicellaChristian AppeltAram ApyanMichaela ArampatziSergio Javier Arbiol ValChiara ArcangelettiAyana Tamu ArceJean-Francois ArguinSpyros ArgyropoulosJan-Hendrik ArlingOlivier ArnaezHannah ArnoldGiacomo ArtoniHaruka AsadaKanae AsaiSiranush AsatryanNedaa Alexandra AsbahRachel Amy Ashby PickeringAsim Mohammed AslamKetevi Adikle AssamaganRobert AstalosSten AstrandRose AtashiRyan Justin AtkinHicham AtmaniPrachi AtmasiddhaKamil AugstenAdrien AuriolVolker Andreas AustrupGiuseppe AvolioKonstantinos AxiotisAmir AzzamDominik BabalHenri BachacouKonstantinos BachasAlexander BachiuErik BachmannMathias Josef BackesAnthony BadeaTamas Marton BaerPaolo BagnaiaMarzieh BahmaniDaniel BahnerKehang BaiJohn BainesLuke BainesKeith BakerEvelin BakosDebottam Bakshi GuptaLuiz Eduardo Balabram FilhoVeena BalakrishnanRahul BalasubramanianEvgenii BaldinPetr BalekEric BallabeneFabrice BalliLisa Marie BaltesWilliam Keaton BalunasJohannes BalzIsaac BamwidhiElzbieta BanasMarilena BandieramonteAnjishnu BandyopadhyayShubham BansalLiron BarakMarawan BarakatElisabetta BarberioDario BarberisMarlon Benoit BarberoMarten Zefanja BarelTeresa BarillariMartin BarisitsTim BarklowPetr BaronDiego BaronToni BaroncelliAlan BarrJackson BarrFernando BarreiroJoao Barreiro Guimaraes da CostaMaura BarrosSergey BarsovFalk BartelsRainer BartoldusAdam Edward BartonPavol BartosAlexander 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FournierHarald FoxPaolo FrancavillaSimone FrancescatoStefano FranchellucciMatteo FranchiniSilvia FranchinoDavid FrancisLuca FrancoLaura FranconiMelissa FranklinGuglielmo FrattariYuval Yitzhak FridJohnny FriendNick FritzscheAlexander FrochDaniel FroidevauxJames FrostYao FuSebastian Julio Fuenzalida GarridoMinori FujimotoKin Yip FungEduardo Furtado De Simas FilhoMarin FurukawaJuan Fuster VerduAnne GaaAlessandro GabrielliAndrea GabrielliPhilipp GadowGuido GagliardiLouis-Guillaume GagnonSafa GaidSean GalantzanJames GallagherElizabeth GallasAxel GallenBruce Joseph GallopKock Kiam GanSanmay GangulyYanyan GaoAli GarabagluFrancisca Garay WallsCarmen GarciaAndrea Garcia AlonsoArianna Gemma Garcia CaffaroJose Enrique Garcia NavarroMiguel Angel Garcia RuizMaurice Garcia-SciveresGwen Llewellyn GardnerRobert William GardnerNicoletta GarelliRocky Bala GargJack GarganChristopher Andrew GarnerCameron Michael GarveyVeritas Katharina GassmannGabriella GaudioViveka GautamPaolo GauzziJan GavranovicIgor 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GustavinoPhillip GutierrezLuis Felipe Gutierrez ZagazetaManuel GutscheChristian GutschowClaire GwenlanCarl GwilliamEven Simonsen HaalandAndrew HaasMartin HabedankCarl HaberHaleh HadavandAbdelhamid HaddadAsma HadefAlina HaganJan Joachim HahnEmil HainesMahsana HaleemJoseph HaleyGregory HallewellKenji HamanoHassane HamdaouiMatthias HamerSalah El Dine HammoudEmily HampshireJingyi HanLiangliang HanLiang HanShuo HanKazunori HanagakiMike HanceDhanush Anil HangalHamza HanifMichael Donald HankJorgen Beck HansenPeter HansenDaigo HaradaTorsten HarenbergSiarhei HarkushaMatthew Leary HarrisYnyr HarrisJack HarrisonNatalie Marie HarrisonPaul Fraser HarrisonMax HartNicole Michelle HartmanNikolai KrugRosie HasanYoji HasegawaFlorian HaslbeckSohaib HassanReiner HauserMatej HaviernikChris HawkesRichard HawkingsYuichiro HayashiDaniel HaydenChristopher Robyn HayesRobin HayesChris HaysJonathan HaysHelen HaywardMingxu HeYajun HeYi HeNathan HeatleyVincent HedbergConstantin HeideggerKim Katrin HeideggerJesse HeilmanSarah HeimTimon HeimJames Geddy HeinleinJochen Jens HeinrichLukas Alexander HeinrichJiri HejbalMarkus HelbigAlexander HeldSimen HellesundCole Michael HellingSten HellmanAna Maria Henriques CorreiaHannah Elizabeth HerdeYesenia Hernandez JimenezLena Maria HerrmannTim HerrmannGregor HertenRalf HertenbergerLuis HervasMoritz HespingNigel HesseyJohannes HesslerMourad HidaouiNihad HidicEwan HillTarje Solberg HillersoyStephen HillierJulia Rose HindsFlorian HinterkeuserMinoru HiroseShigeki HiroseDominic HirschbuehlTom HitchingsBojan HitiJohn David HobbsRadu HobincuNoam Tal HodAnthony HodgesMark HodgkinsonBen HodkinsonAndreas HoeckerDustyn Dean HoferJudith HoferMichael HolzbockBart HommelsVid HomsakBenjamin Paul HonanJae Jin HongTae Min HongBenjamin Henry HoobermanWalter HopkinsMatthew Caleb HoppeschYasuyuki HoriiMalin Elisabeth HorstmannSuen HouMason Ray HousengaJames William HowarthJoaquin HoyaMiroslav HrabovskyTetiana HrynovaPai-Hsien HsuShih-Chieh HsuTao HsuMiao HuQipeng HuShuhui 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JiaZihang JiaCheng JiangQimin JiangStephen JigginsMiguel Jimenez OrtegaJavier Jimenez PenaShan JinAdam JinaruOsamu JinnouchiPer Daniel Conny JohanssonKenneth JohnsJacob JohnsonFiona Ann JollyDominic JonesEleanor JonesKyle Scott JonesPaul JonesRoger JonesTim JonesHans Ludwig JoosRoshan JoshiJelena JovicevicXiangyang JuJohannes JunggeburthThomas JunkermannAurelio Juste RozasMonika Katarzyna JuzekSonia KabanaAnna KaczmarskaSadaf Aliah KadirMarumi KadoHarris KaganMichael KaganAbraham KahnChristian KahraToshiaki KajiEnrique Kajomovitz MustNilotpal KakatiNiraj KakotyIlia KalaitzidouSuman KandelNathan Jihoon KangDeepak KarEfstathios KarentzosKiran KarkiOsama KarkoutSergey KarpovZoya KarpovaVato KartvelishviliAndrey KaryukhinEirini KasimiJudith KatzySandeep KaurKentaro KawadeMayuri Prabhakar KawaleChihiro KawamotoTatsuo KawamotoEllis KayColette KayaStergios KazakosVassili KazaninJames Michael KeaveneyRichard KeelerGustavs KehrisJohn Stakely KellerMitch KellyJacob Julian KempsterOldrich 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KortmanOliver KortnerSandra KortnerWill KosteckaMatus KostovVadim KostyukhinAnastasia KotsokechagiaAshutosh KotwalAimilianos KoulourisAthina Kourkoumeli-CharalampidiChristine KourkoumelisVangelis KourlitisOndrej KovandaBob KowalewskiWitold KozaneckiAnatoli KozhinViktor KramarenkoGregor KrambergerPeter KramerMieczyslaw Witold KrasnyAttila KrasznahorkayJack KrausJohanna Wanda KrausJakub KremerNils Benedikt KrengelTom KresseLukas KretschmannJan KretzschmarPeter KriegerKarol KrizkaKevin Alexander KroeningerHubert KrohaJiri KrollIra Joseph KrollKyle Stuart KrowpmanUladzimir KruchonakHans KruegerNils Erik KrumnackMark KruseOlesia KuchinskaiaSinan KudaySusanne KuehnRoman KustersThorsten KuhlVictor KukhtinYuri KoultchitskiSerguei KuleshovJudith KullEshita Vinay KumarMukesh KumarNeelam KumariPriyanka KumariAlexander KupcoAndrey KupichOleg KuprashHisaya KurashigeLeonid KurchaninovOleksii KurdyshYurii KurochkinAnastasia KurovaMasahiro KuzeAudrey Katherine KvamJiri KvitaNicholas KyriacouCarlos 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des Particules Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire des deux Infinis de Toulouse Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique de Clermont Laboratoire de Physique de Clermont Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules Laboratoire d'Annecy de Physique des Particules Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Centre de Physique des Particules de Marseille Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique Nucléaire et de Hautes Énergies Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique de Clermont Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules Centre de Physique des Particules de Marseille Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Centre de Physique des Particules de Marseille Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille Institut de Recherches sur les lois 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Marseille Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Centre de Physique des Particules de Marseille Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Centre de Physique des Particules de Marseille Laboratoire des deux Infinis de Toulouse Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire des deux Infinis de Toulouse Laboratoire des deux Infinis de Toulouse Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille Laboratoire des deux Infinis de Toulouse Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire des deux Infinis de Toulouse Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Subatomique et de Cosmologie Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire des deux Infinis de Toulouse Laboratoire de Physique des 2 Infinis Irène Joliot-Curie
• Publié dans Eur.Phys.J.C le 30/10/2025

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Résumé : A search for R-parity-conserving supersymmetry in events with large missing transverse momentum, jets and at least one hadronically decaying $τ$-lepton is presented. Both gluino and squark pair production are considered, with the cascade decay of each gluino or squark producing either a $τ$-slepton or a $τ$-sneutrino. Three channels are examined, requiring either exactly one hadronically decaying $τ$-lepton and no other leptons, exactly one hadronically decaying $τ$-lepton and at least one other lepton, or two or more hadronically decaying $τ$-leptons. Analyses in the three channels are optimised independently and combined statistically. Two separate analysis strategies, either a cut-and-count or machine-learning approach, are used. The search uses 140 $\mathrm{fb}^{-1}$ and 51.8 $\mathrm{fb}^{-1}$ of $pp$ collision data recorded by the ATLAS detector at the Large Hadron Collider during 2015-2018 at $\sqrt{s} = 13$ TeV and 2022-2023 at $\sqrt{s} = 13.6$ TeV, respectively. Gluino masses below $2.25$ TeV and squark masses up to $1.7$ TeV are excluded.

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2025
• Auteurs : Ibrahim Jaser AbualrobShreyasi AcharyaGianluca Aglieri RinellaLuca AgliettaMichelangelo AgnelloNeelima AgrawalZubayer AhammedShakeel AhmadIshaan AhujaZulkaida AkbarAlexander AkindinovValentina AkishinaMohammad Al-TuranyDmitry AleksandrovBruno AlessandroHaidar Mas'Ud AlfandaJose Ruben Alfaro MolinaBushra AliAndrea AliciAnton AlkinJohan AlmeGiacomo AloccoTorsten AltAnna Rita AltamuraIgor AltsybeevCristian AndreiNicodemos AndreouAnton AndronicEvgeny AndronovVenelin AnguelovFederico AntinoriPietro AntonioliNicole ApadulaHarald AppelshaeuserSilvia ArcelliRoberta ArnaldiJhoao Gabriel Martins Campos Almeida ArneiroIonut Cristian ArseneMesut ArslandokAndre AugustinusRalf Peter AverbeckMohd Danish AzmiHitoshi BabaAkash Raj John BabuAngela BadalaJoonsuk BaeYunseul BaeYongwook BaekXiaozhi BaiRaphaelle Marie BailhacheYoshini BailungRenu BalaAlberto BaldisseriBartosz BalisShubham BangaliaZarina BanooVeronika BarbasovaFrancesco BarileLuca BarioglioMaria BarlouBanajit BarmanGergely Gabor BarnafoldiLee Stuart BarnbyEmilie Martine BarreauValerie Ramillien BarretLeonardo Barreto de Oliveira CamposKlaus BarthEsther BartschNicole BastidGuillaume BatigneDaniel BattistiniBoris BatyunyaDibakar BauriJose Luis Bazo AlbaIan Gardner BeardenPascal BechtDebadatta BeheraSwadhin BeheraIouri BelikovValerio Di BellaFrancesca BelliniRene BellwiedLucina Gabriela Espinoza BeltranYael Antonio Vasquez BeltranGyula BencediAdel BensaoulaStefania Maria BeoleYaroslav BerdnikovAnastasia BerdnikovaLuisa BergmannLorenzo BernardinisLatchezar BetevPartha Pratim BhaduriTushar BhallaAnju BhasinBuddhadeb BhattacharjeeSumit BhattaraiLivio BianchiJaroslav BielcikJana BielcikovaAnte BilandzicAnna BinoyGabor BiroSaikat BiswasDmitry BlauMihail Bogdan BlidaruNora BluhmeChristoph BlumeFriederike BockTea BodovaJeongsu BokLaszlo BoldizsarMarek BombaraPeter Matthew BondGermano BonomiHerve BorelAlexander BorissovAndres Gerardo Borquez CarcamoElena BottaYoussef El Mard BouzianiDiana Catalina BrandiburLars 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• Organismes : Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique de Clermont Laboratoire de Physique de Clermont Laboratoire de physique subatomique et des technologies associées Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Physique des 2 Infinis de Lyon Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique de Clermont Laboratoire de Physique de Clermont Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Subatomique et de Cosmologie Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique de Clermont Institut de Physique des 2 Infinis de Lyon Institut Pluridisciplinaire Hubert Curien Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique de Clermont Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Physique des 2 Infinis de Lyon Institut Pluridisciplinaire Hubert Curien Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique de Clermont Institut de Physique des 2 Infinis de Lyon Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Physique des 2 Infinis de Lyon Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique de Clermont
• Publié dans JHEP le 14/01/2026

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Résumé : The first measurement at midrapidity ($|y| < 0.5$) of the production yield of the strange-charm baryons $Ξ_c^+$ and $Ξ_c^0$ as a function of charged-particle multiplicity in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ALICE experiment at the LHC is reported. The $Ξ_c^+$ baryon is reconstructed via the $Ξ_c^+ \rightarrow Ξ^-π^+π^+$ decay channel in the range $4 < p_{\rm T} < 12$ GeV/$c$, while the $Ξ_c^0$ baryon is reconstructed via both the $Ξ_c^0 \rightarrow Ξ^-π^+$ and $Ξ_c^0 \rightarrow Ξ^-e^+ν_e$ decay channels in the range $2 < p_{\rm T} < 12$ GeV/$c$. The baryon-to-meson ($Ξ_c^{0,+}/D^0$) and the baryon-to-baryon ($Ξ_c^{0,+}/Λ_c^+$) production yield ratios show no significant dependence on multiplicity. In addition, the observed yield ratios are not described by theoretical predictions that model charm-quark fragmentation based on measurements at $e^+e^-$ and $e^-$p colliders, indicating differences in the charm-baryon production mechanism in pp collisions. A comparison with different event generators and tunings, including different modelling of the hadronisation process, is also discussed. Moreover, the branching-fraction ratio of BR($Ξ_c^0 \rightarrow Ξ^-e^+ν_e$)/BR($Ξ_c^0 \rightarrow Ξ^-π^+$) is measured as 0.825 $\pm$ 0.094 (stat.) $\pm$ 0.081 (syst.). This value supersedes the previous ALICE measurement, improving the statistical precision by a factor of 1.6.

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