Philippe JEAN-PIERRE

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2025
• Auteurs : Roel AaijAhmed Sameh Wagih AbdelmottelebCarlos Abellan BetetaFernando Jesus AbudinénThomas AckernleyAyomide Matthew AdefisoyeBernardo AdevaMarco AdinolfiPatrik Harri AdlarsonChristina AgapopoulouChristine Angela AidalaZiad AjaltouniSimon AkarKazuyoshi AkibaPietro AlbicoccoJohannes AlbrechtFederico AlessioMichael AlexanderZakariya AliouchePaula Alvarez CartelleRenaud AmalricSandra AmatoJake Lewis AmeyY. AmhisLiupan AnLucio AnderliniMartin AnderssonAleksei AndreianovPasquale AndreolaMirco AndreottiDimitra AndreouAlessia AnelliDong AoFlavio ArchilliMatteo ArgentonSergio Arguedas CuendisAlexander ArtamonovMarina ArtusoElie AslanidesRita Ataíde da SilvaMichele AtzeniBenjamin AudurierDavid BacherIrene Bachiller PereaSebastian BachmannMarie BachmayerJohn BackPablo Baladron RodriguezVladislav BalaguraWander BaldiniLuca BalzaniHaoran BaoJuan Baptista de Souza LeiteCarlos Javier Barbero PretelMatteo BarbettiIvanildo Rui BarbosaRoger BarlowMikhail BarnyakovSergey BarsukWilliam BarterMatteo BartoliniJustin BartzJan-Marc BaselsSaliha BashirGiovanni BassiBaasansuren BatsukhPiera BattistaAurelio BayAnja BeckMaik BeckerFranco BedeschiIgnacio BediagaNoah Albin BehlingSamuel BelinViolaine BelleeKonstantin BelousIlia BelovIvan BelyaevGaya BenaneGiovanni BencivenniEli Ben-HaimAlexander BerezhnoyRoland BernetSergi Bernet AndresAlessandro BertolinChristopher BetancourtFederico BettiJosh BexIaroslava 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GalatiMaria Domenica GalatiAbraham Gallas TorreiraDomenico GalliSilvia GambettaMiriam GandelmanPaolo GandiniBilal Ahmad GanieHan GaoRui GaoTian-Qi GaoYang GaoYuanning GaoYuxi GaoMichela GarauLuis Miguel Garcia MartinPaula Garcia MorenoJulián García PardiñasKunal GargLluis GarridoClara GasparRobbert Erik GeertsemaLouis Lenard GerkenEvelina GersabeckMarco GersabeckTimothy GershonSimon GhizzoZahra GhorbanimoghaddamLuca GiambastianiFotis Ioannis GiasemisValerie GibsonHenryk Karol GiemzaAlexander Leon GilmanMatteo GiovannettiAlessandra GioventùLucas George GirardeyPere Gironella GironellCarmen GiuglianoMaciej Artur GizaEvangelos Leonidas GkougkousisFabian Christoph GlaserVladimir GligorovCarla GöbelElisabet GolobardesDmitry GolubkovAndrey GolutvinAlvaro GomesSergio Gomez FernandezFernanda Goncalves AbrantesMateusz GoncerzGuanghua GongJames Andrew GoodingIgor Vladimirovich GorelovClaudio GottiJascha Peter GrabowskiLuis Alberto Granado CardosoEugeni GraugésElena GraveriniLuke GrazetteGiacomo 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Lucio MartinezValeriia LukashenkoYiheng LuoAnna LupatoEleonora LuppiKate LynchXiao-Rui LyuGe MaRuiting MaSerena MaccoliniFrederic MachefertFlorin MaciucBridget MackInnes MackayLauren Grace MackeyLakshan Ram Madhan MohanMarcus Jonathan MaduraiArtem MaevskiyDaniel MagdalinskiDmitrii MaisuzenkoMaciej Witold MajewskiJakub Jacek MalczewskiSneha MaldeLorenzo MalentaccaAlexander MalininTimofei MaltsevGiulia MancaGiampiero MancinelliChiara MancusoRafel Manera EscaleroDaniele ManuzziDaniele MarangottoJean François MarchandRadoslav MarchevskiUmberto MarconiEdoardo MarianiSaverio MarianiCarla Marin BenitoJörg MarksAlexander Mclean MarshallLucas MartelGabriele MartelliGiuseppe MartellottiLoris MartinazzoliMaurizio MartinelliDiego Martinez SantosFernando Martinez VidalAndré MassafferriRosen MatevAbhijit MathadViacheslav MatiuninClara MatteuzziKara Renee MattioliAndrea MauriEmilie MauriceJoan MauricioPierre Paul Louis MayencourtJose Mazorra de CosMichal MazurekMichael MccannLucas McconnellTamaki 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ZengMing ZengChenjia ZhangDongliang ZhangJianyu ZhangLiming ZhangShulei ZhangShunan ZhangYanxi ZhangYuge ZhangYa ZhaoAlina ZharkovaAlexey ZhelezovShuang ZhengXutao ZhengYangheng ZhengTianwen ZhouXiaokang ZhouYixiong ZhouValeriia ZhovkovskaLinxuan ZhuXianglei ZhuXiaoyu ZhuValery ZhukovJiahui ZhuoQuan ZouDavide ZulianiGianluca Zunica
• Organismes : Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Centre de Physique des Particules de Marseille Laboratoire Leprince-Ringuet Laboratoire d'Annecy de Physique des Particules Laboratoire Leprince-Ringuet 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 Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules Laboratoire Leprince-Ringuet Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille Laboratoire de Physique de Clermont Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Centre de Physique des Particules de Marseille Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique de Clermont Laboratoire Leprince-Ringuet 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 Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire Leprince-Ringuet Laboratoire de Physique de Clermont Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Laboratoire de Physique de Clermont Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille Laboratoire de Physique de Clermont Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille Laboratoire Leprince-Ringuet 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 d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire de Physique de Clermont Laboratoire de Physique de Clermont Centre de Physique des Particules de Marseille Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille Laboratoire Leprince-Ringuet Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire Leprince-Ringuet Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie
• Publié dans Journal of High Energy Physics le 23/10/2020

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Résumé : Measurements of $CP$ observables and the CKM angle $\gamma$ are performed in $B^{\pm} \to D K^*(892)^{\pm}$ decays, where $D$ represents a superposition of $D^0$ and $\overline{D}{}^0$ states, using the LHCb dataset collected during Run 1 (2011-2012) and Run 2 (2015-2018). A comprehensive study of this channel is presented with the $D$ meson reconstructed in two-body final states $K^{\pm}\pi^{\mp}$, $K^+K^-$ and $\pi^+\pi^-$; four-body final states $K^{\pm}\pi^{\mp}\pi^{\pm}\pi^{\mp}$ and $\pi^+\pi^-\pi^+\pi^-$; and three-body final states $K^0_{S} \pi^+\pi^-$ and $K^0_{S} K^+ K^-$. This analysis includes the first observation of the suppressed $B^{\pm} \to [\pi^+K^-]_D K^{*\pm}$ and $B^{\pm} \to [\pi^+K^-\pi^+\pi^-]_D K^{*\pm}$ decays. The combined result gives $\gamma=(63\pm 13)^\circ$.

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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 BratrudPeter Braun-MunzingerMarco BregantMichal BrozGiuseppe Eugenio BrunoValentin Dimitrov BuchakchievMatthew Daniel BucklandHenner BueschingStefania BufalinoPaul Alois BuhlerNazar BurmasovEdith Zinhle ButheleziAleksandr BylinkinChristopher Alfred CarrJuan Carlos Cabanillas NorisMaria Fernanda Torres CabreraHelen Louise CainesAlberto CalivaErnesto Calvo VillarJuan Manuel Mejia CamachoPaolo CameriniMaria Teresa CamerlingoFabio de Moraes CanedoStefano CannitoSierra Lisa CantwayMihai CarabasFrancesca CarnesecchiLeopoldo Abranches de CarvalhoJavier Ernesto Castillo CastellanosMatteo CastoldiFabio CatalanoSamuele CattaruzziRebecca CerriIrakli ChakaberiaPritam ChakrabortyJustin Wei Ong ChanSinjini ChandraSylvain ChapelandMarielle ChartierSouvik ChattopadhayMeiyi ChenTiantian ChengCvetan Valeriev CheshkovDavide ChiapparaVasco Miguel Chibante BarrosoDavid Dobrigkeit ChinellatoFabrizio ChinuEmma Sophia ChizzaliJaeyoon ChoSoyeon ChoPeter ChochulaZuzanna Anna ChochulskaDhrubajyoti ChoudhuryPanagiotis ChristakoglouChristian Holm ChristensenPeter ChristiansenTatsuya ChujoMario CiaccoCorrado CicaloGabriele CimadorFederico CindoloGiulia ClaiFabio Filippo ColamariaDomenico ColellaAngelo ColelliManuel ColocciMatteo ConcasGustavo Conesa BalbastreZaida Conesa del ValleGiacomo ContinJesus Guillermo Contreras NunoMaurice CoquetPietro CorteseMauro Rogerio CosentinoFilippo CostaSusanna CostanzaPhilippe CrochetMaciej Marek CzarnynogaAndrea DaineseGautam DangeMeike Charlotte DanischAndrea DanuProttay DasSupriya DasArchita Rani DashSadhana DashAnnalisa de CaroGiacinto de CataldoJan de CuvelandAlessandro de FalcoDaniele de GruttolaNora de MarcoChiara de MartinSalvatore de PasqualeRohaan DebRaffaele del GrandeLuigi Dello StrittoGeovane Grossi Araujo de SouzaPreeti Dhankher LesserDomenico Di BariMarcello Di CostanzoAntonio Di MauroBenedetto Di RuzzaBatoul DiabYanchun DingJanik DitzelRoberto DiviaAlexandru Florin DobrinBenjamin DonigusLars DopperJan Michal DubinskiAndrea DublaPascal DupieuxNatalia DzalaiovaTabea Maria EderRaymond James EhlersFlorian EisenhutRen EjimaDomenico EliaB. ErazmusFrancesca ErcolessiBruno EspagnonGiulio EulisseDavid EvansLaura FabbiettiMattia FagginJulien FaivreFeng FanWenqing FanTao FangAlessandra FantoniMarkus FaselAlessandro FelicielloGrigorii FeofilovArturo Fernandez TellezLucas Ferrandi de OliveiraMarta Bertran FerrerAndrea FerreroChiara FerreroAlessandro FerrettiVictor Jose Gaston FeuillardDmitry FinogeevFiorella FiondaAmanda Nicole FloresSiegfried Valentin FoertschIlya FokinSergey FokinUmberto FolloRobert ForynskiEnrico FragiacomoEszter FrajnaHenrik FribertUlrich FuchsNicola FunicelloChristophe FurgetArtur FursTakahiro FusayasuJens Joergen GaardhoejeMartino GagliardiAlberto Martin Gago MedinaTanu GahlautCarlos Duarte GalvanSarjeeta GamiParaskevi GanotiJose Maria Garabatos CuadradoJosue Martinez GarciaTonatiuh Garcia ChavezEdmundo Javier Garcia-SolisSara GarettiCorrado GargiuloPiotr Jan GasikHari Mohan GaurAmrit GautamMaria Beatriz de Leone GayMarie GermainRoman August GernhaeuserChandrasekhar GhoshMarco GiacaloneGiulia 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ZhuSenjie ZhuYa ZhuAlessandra ZingarettiStefan Cristi ZugravelNicola Zurlo
• 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 Journal of High Energy Physics le 23/10/2020

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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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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2025
• Auteurs : Shreyasi AcharyaApar AgarwalGianluca Aglieri RinellaLuca AgliettaMichelangelo AgnelloNeelima AgrawalZubayer AhammedShakeel AhmadSang Un AhnIshaan AhujaAlexander AkindinovValentina AkishinaMohammad Al-TuranyDmitry AleksandrovBruno AlessandroHaidar Masud AlfandaJose Ruben Alfaro MolinaBushra AliAndrea AliciNegin AlizadehvandchaliAnton AlkinJohan AlmeGiacomo AloccoTorsten AltAnna Rita AltamuraIgor AltsybeevJesus Ricardo Alvarado GarciaMustafa AnaamCristian AndreiNicodemos AndreouAnton AndronicEvgeny AndronovVenelin AnguelovFederico AntinoriPietro AntonioliNicole ApadulaHarald AppelshaeuserCarolina ArataSilvia ArcelliRoberta ArnaldiJhoao Gabriel Martins Campos Almeida ArneiroIonut Cristian ArseneMesut ArslandokAndre AugustinusRalf Peter AverbeckDmitry AveryanovMohd Danish AzmiHitoshi BabaAngela 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 BastidSumit BasuGuillaume BatigneDaniel BattistiniBoris BatyunyaDibakar BauriJose Luis Bazo AlbaIan Gardner BeardenPascal BechtDebadatta BeheraIouri BelikovAilec Bell HechavarriaFrancesca BelliniRene BellwiedSvetlana BelokurovaLucina Gabriela Espinoza BeltranYael Antonio Vasquez BeltranGyula BencediAdel BensaoulaStefania Maria BeoleYaroslav BerdnikovAnastasia BerdnikovaLuisa BergmannLorenzo BernardinisLatchezar BetevPartha Pratim BhaduriAnju BhasinBuddhadeb BhattacharjeeSumit BhattaraiLivio BianchiJaroslav BielcikJana BielcikovaAlexandre Patrick BigotAnte BilandzicAnna BinoyGabor BiroSaikat BiswasNicolas Luc BizeDmitry BlauMihail Bogdan BlidaruNora BluhmeChristoph BlumeFriederike BockTea BodovaJeongsu BokLaszlo BoldizsarMarek BombaraPeter Matthew BondGermano BonomiHerve BorelAlexander BorissovAndres Gerardo Borquez CarcamoElena BottaYoussef El Mard BouzianiDiana Catalina BrandiburLars BratrudPeter Braun-MunzingerMarco BregantMichal BrozGiuseppe Eugenio BrunoValentin Dimitrov BuchakchievMatthew Daniel BucklandDmitry BudnikovHenner BueschingStefania BufalinoPaul Alois BuhlerNazar BurmasovEdith Zinhle ButheleziAleksandr BylinkinSebastian Adam BysiakJuan Carlos Cabanillas NorisMaria Fernanda Torres CabreraHelen Louise CainesAlberto CalivaErnesto Calvo VillarJuan Manuel Mejia CamachoPaolo CameriniMaria Teresa CamerlingoFabio de Moraes CanedoStefano CannitoSierra Lisa CantwayMihai CarabasFrancesca CarnesecchiLeopoldo Abranches de CarvalhoJavier Ernesto Castillo CastellanosMatteo CastoldiFabio CatalanoSamuele CattaruzziRebecca CerriIrakli ChakaberiaPritam ChakrabortySinjini ChandraSylvain ChapelandMarielle ChartierSouvik ChattopadhayMeiyi ChenTiantian ChengCvetan Valeriev CheshkovDavide ChiapparaVasco Miguel Chibante BarrosoDavid Dobrigkeit ChinellatoFabrizio ChinuEmma Sophia ChizzaliJaeyoon ChoSoyeon ChoPeter ChochulaZuzanna Anna ChochulskaDhrubajyoti ChoudhurySubikash ChoudhuryPanagiotis ChristakoglouChristian Holm ChristensenPeter ChristiansenTatsuya ChujoMario CiaccoCorrado CicaloGabriele CimadorFederico CindoloMichael Rudolf CiupekGiulia ClaiFabio Filippo ColamariaJonathan Samuel ColburnDomenico ColellaAngelo ColelliManuel ColocciMatteo ConcasGustavo Conesa BalbastreZaida Conesa del ValleGiacomo ContinJesus Guillermo Contreras NunoMaurice CoquetPietro CorteseMauro Rogerio CosentinoFilippo CostaSusanna CostanzaPhilippe CrochetMaciej Marek CzarnynogaAndrea DaineseGautam DangeMeike Charlotte DanischAndrea DanuProttay DasSupriya DasArchita Rani DashSadhana DashAnnalisa de CaroGiacinto de CataldoJan de CuvelandAlessandro de FalcoDaniele de GruttolaNora de MarcoChiara de MartinSalvatore de PasqualeRohaan DebRaffaele del GrandeLuigi Dello StrittoKyle Christian DevereauxGeovane Grossi Araujo de SouzaPreeti DhankherDomenico Di BariMarcello Di CostanzoAntonio Di MauroBenedetto Di RuzzaBatoul DiabRaul Arteche DiazYanchun DingJanik DitzelRoberto DiviaOeystein DjuvslandUliana DmitrievaAlexandru Florin DobrinBenjamin DonigusJan Michal DubinskiAndrea DublaPascal DupieuxNatalia DzalaiovaTabea Maria EderRaymond James EhlersFlorian EisenhutRen EjimaDomenico EliaB. ErazmusFrancesca ErcolessiBruno EspagnonGiulio EulisseDavid EvansSergey EvdokimovLaura FabbiettiMattia FagginJulien FaivreFeng FanWenqing FanTao FangAlessandra FantoniMarkus FaselGrigorii FeofilovArturo Fernandez TellezLucas Ferrandi de OliveiraMarta Bertran FerrerAndrea FerreroChiara FerreroAlessandro FerrettiVictor Jose Gaston FeuillardVendulka HumlovaDmitry FinogeevFiorella FiondaFernando Antonio FlorAmanda Nicole FloresSiegfried Valentin FoertschIlya FokinSergey FokinUmberto FolloEnrico FragiacomoEszter FrajnaHenrik FribertUlrich FuchsNicola FunicelloChristophe FurgetArtur FursTakahiro FusayasuJens Joergen GaardhoejeMartino GagliardiAlberto Martin Gago MedinaTanu GahlautCarlos Duarte GalvanSarjeeta GamiDhevan Raja GangadharanParaskevi GanotiJose Maria Garabatos CuadradoJosue Martinez GarciaTonatiuh Garcia ChavezEdmundo Javier Garcia-SolisSara GarettiCorrado GargiuloPiotr Jan GasikHari Mohan GaurAmrit GautamMaria Beatriz de Leone GayMarie GermainRoman August GernhaeuserChandrasekhar 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• Organismes : Laboratoire de Physique Subatomique et de Cosmologie 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 Laboratoire de physique subatomique et des technologies associées 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 Institut de Recherches sur les lois Fondamentales de l'Univers 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 de Physique des 2 Infinis de Lyon 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 Institut de Recherches sur les lois Fondamentales de l'Univers 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 Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique de Clermont
• Publié dans Journal of High Energy Physics le 23/10/2020

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Résumé : Correlations among conserved quantum numbers, such as the net-electric charge, the net-baryon, and the net-strangeness in heavy-ion collisions, are crucial for exploring the QCD phase diagram. In this letter, these correlations are investigated using net-proton number (as a proxy for the net-baryon), net-kaon number (for the net-strangeness), and net-charged particle number in Pb-Pb collisions at $\sqrt{s_\text{NN}}=5.02$ TeV with the ALICE detector. The observed correlations deviate from the Poissonian baseline, with a more pronounced deviation at LHC energies than at RHIC. Theoretical calculations of the Thermal-FIST hadron resonance gas model, HIJING, and EPOS LHC event generators are compared with experimental results, where a significant impact of resonance decays is observed. Thermal-FIST calculations under the grand canonical and canonical ensembles highlight significant differences, underscoring the role of local charge conservation in explaining the data. Recent lattice QCD studies have demonstrated that the magnetic field generated by spectator protons in heavy-ion collisions affects susceptibility ratios, in particular those related to the net-electric charge and the net-baryon numbers. The experimental findings are in qualitative agreement with the expectations of lattice QCD.

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2025
• Auteurs : Shreyasi AcharyaDagmar AdamovaAlexander AdlerGianluca Aglieri RinellaMichelangelo AgnelloNeelima AgrawalZubayer AhammedShakeel AhmadSang Un AhnIshaan AhujaAlexander AkindinovMohammad Al-TuranyDmitry AleksandrovBruno AlessandroHaidar Masud AlfandaJose Ruben Alfaro MolinaBushra AliYasir AliAndrea AliciNegin AlizadehvandchaliAnton AlkinJohan AlmeGiacomo AloccoTorsten AltIgor AltsybeevJesus Ricardo Alvarado GarciaMustafa AnaamCristian AndreiAnton AndronicVenelin AnguelovFederico AntinoriPietro AntonioliAnuj ChandraNicole ApadulaL AphecetcheHarald AppelshaeuserCarolina ArataSilvia ArcelliMauro ArestiRoberta ArnaldiIonut Cristian ArseneMesut ArslandokAndre AugustinusRalf Peter AverbeckMohd Danish AzmiAngela BadalaYongwook BaekXiaozhi BaiRaphaelle Marie BailhacheYoshini BailungRenu BalaAlessandro BalbinoAlberto BaldisseriBartosz BalisDebjani BanerjeeZarina BanooRoberto BarberaFrancesco BarileLuca BarioglioMaria BarlouGergely Gabor BarnafoldiLee Stuart BarnbyValerie Ramillien BarretLeonardo Barreto de Oliveira CamposClara BartelsKlaus BarthEsther BartschFilippo BaruffaldiNicole BastidSumit BasuGuillaume BatigneDaniel BattistiniBoris BatyunyaDibakar BauriJose Luis Bazo AlbaIan Gardner BeardenCaitlin BeattiePascal BechtDebadatta BeheraIouri BelikovAilec Bell HechavarriaFrancesca BelliniRene BellwiedSvetlana BelokurovaVladimir BelyaevGyula BencediStefania Maria BeoleAlexandru BercuciYaroslav BerdnikovAnastasia BerdnikovaLuisa BergmannMihaela Gabriela BesoiuLatchezar BetevPartha Pratim BhaduriAnju BhasinMohammad Asif BhatBuddhadeb BhattacharjeeLivio BianchiNicola BianchiJaroslav BielcikJana BielcikovaJacek Bogumil BiernatAlexandre Patrick BigotAnte BilandzicGabor BiroSaikat BiswasNicolas Luc BizeJustin Thomas BlairDmitry BlauMihail Bogdan BlidaruNora BluhmeChristoph BlumeGianluigi BocaFriederike BockTea BodovaAlexey BogdanovStefano BoiJeongsu BokLaszlo BoldizsarAlexander BolozdynyaMarek 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 BufalinoOphelie BugnonPaul Alois BuhlerEdith Zinhle ButheleziJamila Bashir ButtSebastian Adam BysiakMengke CaiHelen Louise CainesAlberto CalivaErnesto Calvo VillarJuan Manuel Mejia CamachoPaolo CameriniFabio de Moraes CanedoSierra Lisa WeyhmillerMihai CarabasAitor Amatriain CarballoFrancesca CarnesecchiRobin Albert Andre CaronJavier Ernesto Castillo CastellanosFabio CatalanoCesar Ceballos SanchezIrakli ChakaberiaPritam ChakrabortySinjini ChandraSylvain ChapelandMarielle ChartierSubhasis ChattopadhyaySukalyan ChattopadhyayTiantian ChengCvetan Valeriev CheshkovBrigitte CheynisVasco Miguel Chibante BarrosoDavid Dobrigkeit ChinellatoEmma Sophia ChizzaliJaeyoon ChoSoyeon ChoPeter ChochulaPanagiotis ChristakoglouChristian Holm ChristensenPeter ChristiansenTatsuya ChujoMario CiaccoCorrado CicaloLuisa CifarelliFederico CindoloMichael Rudolf CiupekGiulia ClaiFabio Filippo ColamariaJonathan Samuel ColburnDomenico ColellaManuel ColocciMatteo ConcasG. Conesa BalbastreZaida Conesa del ValleGiacomo ContinJesus Guillermo Contreras NunoMaurice CoquetThomas Michael CormierPietro CorteseMauro Rogerio CosentinoFilippo CostaSusanna CostanzaJana CrkovskaPhilippe CrochetReynier Cruz TorresEleazar Cuautle FloresPengyao CuiLeticia Cunqueiro MendezAndrea DaineseMeike Charlotte DanischAndrea DanuProttay DasProttoy DasSupriya DasArchita Rani DashSadhana DashAnnalisa de CaroGiacinto de CataldoJan de CuvelandAlessandro de FalcoDaniele de GruttolaNora de MarcoChiara de MartinSalvatore de PasqualeSuman DebRoman Jan DebskiKamil Rafal DejaRaffaele del GrandeLuigi Dello StrittoWenjing DengPreeti DhankherDomenico Di BariAntonio Di MauroRaul Arteche DiazThomas DietelYanchun DingRoberto DiviaDhruv Utpalkumar DixitOeystein DjuvslandUliana DmitrievaAlexandru Florin DobrinBenjamin DonigusAnand Kumar DubeyJan Michal DubinskiAndrea DublaSandeep DudiPascal DupieuxMartin DurkacNatalia DzalaiovaTabea Maria EderRaymond James EhlersViljar Nilsen EikelandFlorian EisenhutDomenico EliaB. ErazmusFrancesca ErcolessiFilip ErhardtMagnus Rentsch ErsdalBruno EspagnonGiulio EulisseDavid EvansSergey EvdokimovLaura FabbiettiMattia FagginJ. FaivreFeng FanWenqing FanAlessandra FantoniMarkus FaselPietro FecchioAlessandro FelicielloGrigorii FeofilovArturo Fernandez TellezMarta Bertran FerrerAndrea FerreroChiara FerreroAlessandro FerrettiVictor Jose Gaston FeuillardVendulka FilovaDmitry FinogeevFiorella FiondaFernando Antonio FlorAmanda Nicole FloresSiegfried Valentin FoertschIlya FokinSergey FokinEnrico FragiacomoEszter FrajnaUlrich FuchsNicola FunicelloChristophe FurgetArtur FursTakahiro FusayasuJens Joergen GaardhoejeMartino GagliardiAlberto Martin Gago MedinaCarlos Duarte GalvanDhevan Raja GangadharanParaskevi GanotiJose Maria Garabatos CuadradoTonatiuh Garcia ChavezEdmundo Javier Garcia-SolisKunal GargCorrado GargiuloAydan GaribliKatharina DemmichPiotr Jan GasikAmrit GautamMaria Beatriz de Leone GayMarie GermainChandrasekhar GhoshSanjay Kumar GhoshMarco GiacalonePaola GianottiPaolo GiubellinoPiero GiubilatoAude Marie Camille GlaenzerPeter GlasselEwa GlimosDaniel Jia Qin GohVictor Luis Gonzalez SebastianLaura Helena 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KhanAlexei KhanzadeevYury KharlovAnisa KhatunArvind KhuntiaBjarte KilengBeomkyu KimChong KimDong Jo KimEun Joo KimJaehyun KimJinsook KimJiyoung KimJunlee KimMinjung KimSe Yong KimTaejun KimKento KimuraStefan KirschIvan KiselSergey KiselevAdam Ryszard KisielJacek Pawel KitowskiJennifer Lynn KlayJochen KleinSpencer Robert KleinChristian Klein-BoesingMatthias KleinerThomas KlemenzAlexander KlugeAnders Garritt KnospeChinorat KobdajThorsten Sven KolleggerAndrey KondratyevEvgeny KondratyukJoshua Leon KonigStephan Alexander KonigstorferPiotr Jan KonopkaGeorgui Kornakov VanSebastian Dominik KoryciakArtem KotliarovVladimir KovalenkoMarek KowalskiVenelin Valeriev KozhuharovIvan KralikAdela KravcakovaLukas KreisMarian KrivdaFilip KrizekKatarina Krizkova GajdosovaMartin KroesenMario KrugerDiana Maria KrupovaEvgeny KryshenVit KuceraChristian Claude KuhnPaulus Gerardus KuijerTakuya KumaokaDeekshit KumarLokesh KumarNavneet KumarShyam KumarSourav KunduPodist KurashviliAlexander KurepinAlexey 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MankoFranck MansoVito ManzariYaxian MaoGiacomo Vito MargagliottiAnselmo MargottiAna Maria MarinChristina MarkertPaolo MartinengoJacobb Lee MartinezMario Ivan Martinez HernandezGines Martinez-GarciaSilvia MasciocchiMassimo MaseraAlberto MasoniLaure Marie MassacrierAnnalisa MastroserioAndreas Michael MathisOliver MatonohaPaula Fernanda Toledo MatuokaAdam Tomasz MatyjaChristoph MayerAntonio Lafuente MazuecosFrancesco MazzaschiMarianna MazzilliJoyful Elma MdhluliAdrian Florin MechlerYury MelikyanArturo Alejandro Menchaca-RochaElisa MeninnoAnjaly Sasikumar MenonMichal MeresSibaliso MhlangaYasuo MiakeLuca MichelettiLucrezia Camilla MigliorinDimitar Lubomirov MihaylovKonstantin MikhaylovAditya Nath MishraDariusz Czeslaw MiskowiecAbhi ModakAuro Prasad MohantyBedangadas MohantyMohammed Mohisin KhanMikael Andreas MolanderZuzana MoravcovaCindy MordasiniDenise Aparecida Moreira de Godoy WillemsIgor MorozovAndreas MorschTeo MrnjavacValeria MucciforaSanjib MuhuriJames Declan MulliganAlice 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• Organismes : Laboratoire de Physique de Clermont Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique Subatomique et de Cosmologie Institut de Recherches sur les lois Fondamentales de l'Univers 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 Laboratoire de physique subatomique et des technologies associées Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de physique subatomique et des technologies associées 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 Physique des 2 Infinis de Lyon Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique de Clermont Institut de Physique des 2 Infinis de Lyon 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 subatomique et des technologies associées Laboratoire de physique subatomique et des technologies associées Institut de Recherches sur les lois Fondamentales de l'Univers 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 de Physique des 2 Infinis de Lyon Institut Pluridisciplinaire Hubert Curien Institut Pluridisciplinaire Hubert Curien Laboratoire de Physique de Clermont Institut Pluridisciplinaire Hubert Curien Laboratoire de Physique de Clermont Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Institut de Physique des 2 Infinis de Lyon 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 des technologies associées Laboratoire de physique subatomique et des technologies associées Laboratoire de Physique de Clermont Institut de Recherches sur les lois Fondamentales de l'Univers Institut Pluridisciplinaire Hubert Curien Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de physique subatomique et des technologies associées Institut Pluridisciplinaire Hubert Curien 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 de Clermont Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Institut de Physique des 2 Infinis de Lyon Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Institut de Recherches sur les lois Fondamentales de l'Univers
• Publié dans Nucl.Phys.B le 22/01/2026

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Résumé : The measurement of $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) yields as a function of the charged-particle multiplicity density, $\textrm{d}N_{\textrm{ch}}/\textrm{d}\eta$, using the ALICE experiment at the LHC, is reported in pp collisions at $\sqrt{s} =$ 13 TeV. The $\Upsilon$ meson yields are measured at forward rapidity ($2.5 < y < 4$) in the dimuon decay channel, whereas the charged-particle multiplicity is defined at central rapidity ($|\eta| < 1$). Both quantities are divided by their average value in minimum bias events to compute the self-normalized quantities. The increase of the self-normalized $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) yields is found to be compatible with a linear scaling with the self-normalized $\textrm{d}N_{\textrm{ch}}/\textrm{d}\eta$, within the uncertainties. The self-normalized yield ratios of excited-to-ground $\Upsilon$ states are compatible with unity within uncertainties. Similarly, the measured double ratio of the self-normalized $\Upsilon$(1S) to the self-normalized J/$\psi$ yields, both measured at forward rapidity, is compatible with unity for self-normalized charged-particle multiplicities beyond one. The measurements are compared with theoretical predictions incorporating initial or final state effects.

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