Philippe JEAN-PIERRE

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2024
• Auteurs : Marine CholinCécile GenevoisPierre CarlesMathieu AllixJulie CornetteMaggy ColasFranck FayonVincent Sarou-KanianGaelle DelaizirPhilippe ThomasSébastien ChenuVincent CoudercJ.-R. Duclère
• Organismes : XLIM IRCER - Axe 3 : organisation structurale multiéchelle des matériaux Conditions Extrêmes et Matériaux : Haute Température et Irradiation Institut de Recherche sur les CERamiques Conditions Extrêmes et Matériaux : Haute Température et Irradiation IRCER - Axe 3 : organisation structurale multiéchelle des matériaux IRCER - Axe 3 : organisation structurale multiéchelle des matériaux Conditions Extrêmes et Matériaux : Haute Température et Irradiation Conditions Extrêmes et Matériaux : Haute Température et Irradiation IRCER - Axe 3 : organisation structurale multiéchelle des matériaux IRCER - Axe 3 : organisation structurale multiéchelle des matériaux Institut des Sciences Chimiques de Rennes IRCER - Axe 3 : organisation structurale multiéchelle des matériaux Université de Limoges XLIM IRCER - Axe 3 : organisation structurale multiéchelle des matériaux
• Publié dans Crystal Growth & Design le 31/10/2020

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Résumé : The molar composition 30TeO2–40B2O3–30Bi2O3 doped with 0.5Er2O3 is explored. Starting from a homogeneous glass, new borotellurite glass-ceramics were elaborated after a two-step heat treatment composed of both nucleation and growth processes. The crucial parameters, determined by differential scanning calorimetry, were the nucleation optimal temperature and duration. The structural modifications occurring while heating and the related microstructure evolution were followed by ex situ X-ray Diffraction and Scanning Electron Microscopy. Mechanisms of the partial crystallization were investigated through Transmission Electron Microscopy observations and local chemical analyses (Energy Dispersive Spectroscopy and Electron Energy Loss Spectroscopy). Thus, the employed heat treatments formed glass-ceramics composed of boron-free Bi2Te2O7 polycrystalline entities dispersed in the boron-oxide-enriched glassy matrix. The partial crystallization happens, therefore, concomitantly with the observed chemical demixtion, where boron oxide separates from the bismuth tellurite phase. Additionally, Raman spectroscopy and Nuclear Magnetic Resonance data reveal that the overall BO4/BO3 ratio of the glass network does not show significant evolution during the partial crystallization. Optical transmission and photoluminescence properties were also measured. For glass-ceramics, the optical transmission strongly drops. Both emission and excitation spectra of Er3+ ions, as well as lifetime measurements, highlight the modified environment around the rare-earth ions occurring with partial crystallization.

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Fichiers liés : Cholin 2024 Crystallization Mechanisms in New Bismuth Borotellurite Glass-Ceramics _Crystal_Growth_Design_submitted_version.pdf

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• Type de publi. : Rapport
• Date de publi. : 01/01/2024
• Auteurs : Noémie EtienneJean-Philippe BedellJean-Luc Bertrand-KrajewskiPierre BenoitElodie BrelotChristophe DagotDominique PatureauAlexandra PinsclouxLaure Wiest
• Organismes : Déchets Eaux Environnement Pollutions École Nationale des Travaux Publics de l'État Déchets Eaux Environnement Pollutions Institut National de Recherche pour l’Agriculture, l’Alimentation et l’Environnement Groupe de Recherche Rhône Alpes sur les Infrastructures et l'Eau Université de Limoges Institut National de Recherche pour l’Agriculture, l’Alimentation et l’Environnement Groupe de Recherche Rhône Alpes sur les Infrastructures et l'Eau Institut des Sciences Analytiques

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Fichiers liés : AP-N 092 Etienne et al 2024 Synthese_Programme_Rismeau_2019_2023.pdf

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2024
• Auteurs : Shreyasi AcharyaDagmar AdamovaAlexander AdlerGianluca 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 BarlouGergely 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 BelokurovaGyula 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 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 ChochulaPanagiotis ChristakoglouChristian Holm ChristensenPeter ChristiansenTatsuya ChujoMario CiaccoCorrado CicaloFederico CindoloMichael Rudolf CiupekGiulia ClaiFabio Filippo ColamariaJonathan Samuel ColburnDomenico ColellaManuel ColocciMatteo ConcasG. 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VilakaziOrlando Villalobos BaillieAnna VillaniGioacchino VinoAlexander VinogradovTiziano VirgiliMaxim Mikael Olavi VirtaVytautas VislaviciusAlexander VodopyanovBenedikt VoelkelMartin Andreas VolklKirill VoloshinSergey VoloshinGiacomo VolpeBarthelemy von HallerIvan VorobyevNikita VozniukJanka VrlakovaJie WanChunzheng WangDongfang WangYuanzhe WangYubiao WangAdam Tadeusz WegrzynekFelix Thomas WeiglhoferSandro Christian WenzelJohannes Peter WesselsSierra Lisa WeyhmillerJens WiechulaJon WikneGrzegorz Andrzej WilkJeremy John WilkinsonGuido Alexander WillemsBernd Stefan WindelbandMichael Andreas WinnJosephina Rae WrightWenya WuYitao WuRan XuAnkur YadavArun Kumar YadavSerpil Yalcin KuzuYorito YamaguchiShiming YangSatoshi YanoZhongbao YinIn Kwon YooJin Hee YoonHyeonjin YuShiming YuanAlperen YuncuValentina ZaccoloChiara ZampolliFederica ZanoneNima ZardoshtiAndrey ZarochentsevPetr ZavadaNikolay ZavyalovMikhail ZhalovBiao ZhangChi ZhangLiuyao ZhangSong ZhangXiaoming ZhangYifei ZhangZhen ZhangMingrui ZhaoVladimir ZherebchevskiiZhi YuDaicui ZhouYou ZhouJianhui ZhuYa ZhuStefan Cristi ZugravelNicola Zurlo
• 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 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 des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Institut de Recherches sur les lois Fondamentales de l'Univers 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 de Clermont 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 Institut de Physique des 2 Infinis de Lyon 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 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 des 2 Infinis Irène Joliot-Curie 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 Recherches sur les lois Fondamentales de l'Univers
• Publié dans JHEP le 14/01/2026

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Résumé : Measurements of inclusive charged-particle jet production in pp and p-Pb collisions at center-of-mass energy per nucleon-nucleon collision $\sqrt{s_{\rm NN}} = 5.02$ TeV and the corresponding nuclear modification factor $R_{\rm pPb}^{\rm ch\,jet}$ are presented, using data collected with the ALICE detector at the LHC. Jets are reconstructed in the central rapidity region $|\eta_{\rm jet}| < 0.5$ from charged particles using the anti-$k_{\rm T}$ algorithm with resolution parameters $R = 0.2$, 0.3, and 0.4. The $p_{\rm T}$-differential inclusive production cross section of charged-particle jets, as well as the corresponding cross-section ratios, are reported for pp and p-Pb collisions in the transverse momentum range $10 < p^{\rm ch}_{\rm T,jet} < 140$ GeV/$c$ and $10 < p^{\rm ch}_{\rm T,jet} < 160$ GeV/$c$, respectively, together with the nuclear modification factor $R_{\rm pPb}^{\rm ch\,jet}$ in the range $10 < p^{\rm ch}_{\rm T,jet} < 140$ GeV/$c$. The analysis extends the $p_{\rm T}$ range of the previously-reported charged-particle jet measurements by the ALICE Collaboration. The nuclear modification factor is found to be consistent with one and independent of the jet resolution parameter with the improved precision of this study, indicating that the possible influence of cold nuclear matter effects on the production cross section of charged-particle jets in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV is smaller than the current precision. The obtained results are in agreement with other minimum bias jet measurements available for RHIC and LHC energies, and are well reproduced by the NLO perturbative QCD POWHEG calculations with parton shower provided by PYTHIA8 as well as by JETSCAPE simulations.

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Fichiers liés : JHEP05(2024)041.pdf

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Source

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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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• 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 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 des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Institut de Recherches sur les lois Fondamentales de l'Univers 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 de Clermont 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 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 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 des 2 Infinis Irène Joliot-Curie 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 Recherches sur les lois Fondamentales de l'Univers
• Publié dans JHEP le 14/01/2026

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Résumé : The ALICE Collaboration reports a search for jet quenching effects in high-multiplicity (HM) proton$-$proton collisions at $\sqrt{s}$ = 13 TeV, using the semi-inclusive azimuthal-difference distribution $\Delta\varphi$ of charged-particle jets recoiling from a high transverse momentum (high-$p_{\mathrm{T,trig}}$) trigger hadron. Jet quenching may broaden the $\Delta\varphi$ distribution measured in HM events compared to that in minimum bias (MB) events. The measurement employs a $p_{\mathrm{T,trig}}$-differential observable for data-driven suppression of the contribution of multiple partonic interactions, which is the dominant background. While azimuthal broadening is indeed observed in HM compared to MB events, similar broadening for HM events is observed for simulations based on the PYTHIA 8 Monte Carlo generator, which does not incorporate jet quenching. We elucidate the origin of the broadening by comparing biases induced by HM selection in the data and simulations, and discuss its implications for the study of jet quenching in small collision systems.

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Fichiers liés : JHEP05(2024)229.pdf

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2024
• Auteurs : Shreyasi AcharyaDagmar AdamovaAlexander AdlerGianluca 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 AltIgor AltsybeevJesus Ricardo Alvarado GarciaMustafa AnaamCristian AndreiAnton AndronicVenelin AnguelovFederico AntinoriPietro AntonioliNicole ApadulaL AphecetcheHarald AppelshaeuserCarolina ArataSilvia ArcelliMauro ArestiRoberta ArnaldiJhoao Gabriel Martins Campos Almeida ArneiroIonut Cristian ArseneMesut ArslandokAndre AugustinusRalf Peter AverbeckMohd Danish AzmiAngela BadalaJoonsuk BaeYongwook BaekXiaozhi BaiRaphaelle Marie BailhacheYoshini BailungAlessandro BalbinoAlberto BaldisseriBartosz BalisDebjani BanerjeeZarina BanooRoberto BarberaFrancesco BarileLuca BarioglioMaria BarlouGergely 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 BelokurovaVladimir BelyaevGyula 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 Luc BizeJustin 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 BuhlerEdith Zinhle ButheleziAleksandr BylinkinSebastian Adam BysiakMengke CaiHelen Louise CainesAlberto CalivaErnesto Calvo VillarJuan Manuel Mejia CamachoPaolo CameriniFabio de Moraes CanedoSierra Lisa WeyhmillerMihai CarabasAitor Amatriain CarballoFrancesca CarnesecchiRobin Albert Andre CaronLeopoldo Abranches de CarvalhoJavier 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 CicaloFederico CindoloMichael Rudolf CiupekGiulia ClaiFabio Filippo ColamariaJonathan Samuel ColburnDomenico ColellaManuel ColocciMatteo ConcasG. Conesa BalbastreZaida Conesa del ValleGiacomo ContinJesus Guillermo Contreras NunoMaurice Louis CoquetThomas Michael CormierPietro CorteseMauro Rogerio CosentinoFilippo CostaSusanna CostanzaCorentin CotJana CrkovskaPhilippe CrochetReynier Cruz TorresPengyao CuiAndrea 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 PasqualeRohaan DebSuman DebRoman Jan DebskiKamil Rafal DejaRaffaele del GrandeLuigi Dello StrittoWenjing DengPreeti DhankherDomenico Di BariAntonio Di MauroBatoul DiabRaul Arteche DiazThomas DietelYanchun DingRoberto DiviaDhruv Utpalkumar DixitOeystein DjuvslandUliana DmitrievaAlexandru Florin DobrinBenjamin DonigusJan Michal DubinskiAndrea DublaSandeep DudiPascal DupieuxMartin DurkacNatalia DzalaiovaTabea Maria EderRaymond James EhlersFlorian EisenhutDomenico EliaB. 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ZugravelNicola Zurlo
• 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 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 des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Institut de Recherches sur les lois Fondamentales de l'Univers 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 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 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 Institut de Recherches sur les lois Fondamentales de l'Univers
• Publié dans Phys.Lett.B le 31/10/2025

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Résumé : The ALICE Collaboration reports a differential measurement of inclusive jet suppression using pp and Pb–Pb collision data at a center-of-mass energy per nucleon–nucleon collision sNN=5.02 TeV. Charged-particle jets are reconstructed using the anti-kT algorithm with resolution parameters R=0.2, 0.3, 0.4, 0.5, and 0.6 in pp collisions and R=0.2, 0.4, 0.6 in central (0–10%), semi-central (30–50%), and peripheral (60–80%) Pb–Pb collisions. A novel approach based on machine learning is employed to mitigate the influence of jet background. This enables measurements of inclusive jet suppression in new regions of phase space, including down to the lowest jet pT≥40 GeV/c at R=0.6 in central Pb–Pb collisions. This is an important step for discriminating different models of jet quenching in the quark–gluon plasma. The transverse momentum spectra, nuclear modification factors, derived cross section, and nuclear modification factor ratios for different jet resolution parameters of charged-particle jets are presented and compared to model predictions. A mild dependence of the nuclear modification factor ratios on collision centrality and resolution parameter is observed. The results are compared to a variety of jet-quenching models with varying levels of agreement.

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Fichiers liés : 1-s2.0-S0370269323007451-main.pdf

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