Philippe JEAN-PIERRE

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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 GarciaCesar Omar Ramirez AlvarezMustafa AnaamCristian AndreiNicodemos AndreouAnton AndronicEvgeny AndronovVenelin AnguelovFederico AntinoriPietro AntonioliNicole ApadulaL AphecetcheHarald 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 BalisZarina BanooVeronika BarbasovaFrancesco BarileLuca BarioglioMaria BarlouBanajit BarmanGergely Gabor BarnafoldiLee Stuart BarnbyEmilie Martine BarreauValerie 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 BelokurovaLucina Gabriela Espinoza BeltranYael Antonio Vasquez BeltranGyula BencediAdel BensaoulaStefania Maria BeoleYaroslav BerdnikovAnastasia BerdnikovaLuisa BergmannMihaela Gabriela BesoiuLatchezar BetevPartha Pratim BhaduriAnju BhasinBuddhadeb BhattacharjeeLivio BianchiJaroslav BielcikJana BielcikovaAlexandre Patrick BigotAnte BilandzicAnna BinoyGabor BiroSaikat BiswasNicolas Luc BizeJustin Thomas BlairDmitry BlauMihail Bogdan BlidaruNora BluhmeChristoph BlumeFriederike BockTea BodovaJeongsu BokLaszlo 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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 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 Physique des 2 Infinis de Lyon 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 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 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 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 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 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 Phys.Rev.C le 31/10/2025

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Résumé : The first measurements of proton emission accompanied by neutron emission in the electromagnetic dissociation (EMD) of $^{208}$Pb nuclei in the ALICE experiment at the LHC are presented. The EMD protons and neutrons emitted at very forward rapidities are detected by the proton and neutron Zero Degree Calorimeters of the ALICE experiment. The emission cross sections of zero, one, two, and three protons accompanied by at least one neutron were measured in ultraperipheral $^{208}$Pb-$^{208}$Pb collisions at a center-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}=5.02$~TeV. These 0p, 1p, 2p, and 3p cross sections are described by the RELDIS model, and according to this model, they are associated with the production of various isotopes of Pb, Tl, Hg, and Au in the EMD of $^{208}$Pb. The cross sections of the emission of a single proton accompanied by the emission of one, two, or three neutrons in EMD were also measured. The data are significantly overestimated by the RELDIS model, which predicts that the (1p,1n), (1p,2n), and (1p,3n) cross sections are very similar to the cross sections for the production of the thallium isotopes $^{206,205,204}$Tl.

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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 AmeyYasmine 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 BalaguraAnna BalboniWander 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 BezshyikoJihyun BhomMartin Stefan BiekerNicolo Vladi BiesuzPierre BilloirAlice BiolchiniMatthew BirchFionn Caitlin Ros BishopAlexander BitadzeAndrea BizzetiThomas BlakeFrederic BlancJonah Evan BlankSteven BluskVladimir BocharnikovJulian Alexander BoelhauveOscar Boente GarciaThomas BoettcherAbhishek BohareAlexey BoldyrevCarolina BolognaniRiccardo BolzonellaRiccardo BonacciNikolay BondarAleksandar BordeliusFederica BorgatoSilvia BorghiMartino BorsatoJozef Tomasz BorsukSonia Amina BouchibaMarcelo BovillThemistocles BowcockAlexandre BoyerConcezio BozziAlexandre Brea RodriguezNils BreerJolanta BrodzickaArnau Brossa GonzaloJames David BrownDavide BrunduEmma BuchananAnnarita BuonauraLaura BuonincontriAodhan Tomas BurkeChristopher BurrJordy Sebastiaan ButterJan BuytaertWiktor ByczynskiSandro CadedduHao CaiAlois CailletRoberto CalabreseSaul Calderon RamirezLukas CaleficeStefano CaliMarta CalviMiriam Calvo GomezPatricia Camargo MagalhaesJose Ivan Cambon BouzasPierluigi CampanaDaniel Hugo Campora PerezAngel Fernando Campoverde QuezadaSimone CapelliLorenzo CapriottiRonald Gerardo Caravaca-MoraAngelo CarboneLidia Carcedo SalgadoRoberta CardinaleAlessandro CardiniPaolo CarnitiLeon David CarusAdrian Casais VidalRowina CasparyGianluigi CasseMarco CattaneoGiovanni CavalleroViola CavalliniSara CelaniDaniel CervenkovSara CesareAbbie Jane ChadwickIbrahim ChahrourMatthew CharlesPhilippe CharpentierEvridki ChatzianagnostouMaximilien ChefdevilleChen ChenShanzhen ChenZewen ChenAleksei ChernovSerhii ChernyshenkoXenofon ChiotopoulosVeronika ChobanovaSerhii 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Gironella GironellCarmen GiuglianoMaciej Artur GizaEvangelos Leonidas GkougkousisFabian Christoph GlaserVladimir GligorovCarla GöbelElisabet GolobardesDmitry GolubkovAndrey GolutvinSergio Gomez FernandezWojciech GomulkaFernanda Goncalves AbrantesMateusz GoncerzGuanghua GongJames Andrew GoodingIgor Vladimirovich GorelovClaudio GottiJascha Peter GrabowskiLuis Alberto Granado CardosoEugeni GraugésElena GraveriniLuke GrazetteGiacomo GrazianiAlexandru Tudor GrecuLex Marinus GreevenNathan Allen GrieserLucia GrilloSergey GromovChenxi GuMarco GuariseLaetitia GuerryManuel GuittiereVasilisa GuliaevaPaul Andre GüntherAbdul-Kerim GuseinovEvgeny GushchinYury GuzThierry GysKai Sebastian HabermannThomas HadavizadehChristos HadjivasiliouGuido HaefeliChristophe HaenJakob HaimbergerMohammadtaghi HajheidariGeorge HallettMarius Maehlum HalvorsenPhoebe Meredith HamiltonJan HammerichQundong HanXiaoxue HanStephanie Hansmann-MenzemerLei HaoNeville HarnewMarie HartmannSabin HashmiJibo HeFrederic HemmerConor HendersonRiley Dylan Leslie HendersonArthur Marius HennequinKarol HennessyLouis HenryJames Daniel HerdPaula Herrero GasconJohannes HeuelAdlène HicheurGuillermo Hijano MendizabalDonal HillJoshua Ethan HorswillRuiwen HouYingrui HouNed Francis HowarthJifeng HuWenhua HuXiaofan HuWenqian HuangWouter HulsbergenRoss John HunterMikhail HushchynDavid HutchcroftMarek IdzikDmitrii IlinPhilip IltenAlexander InglessiAleksandr IniukhinArtur IshteevKuzma IvshinRichard JacobssonHendrik JageSergio Javier Jaimes EllesSune JakobsenEddy JansBrij Kishor JashalAbolhassan JawaheryVukan JevticEmily Kaiyin JiangXiaojie JiangYi JiangYuyang JiangMalcolm JohnAllen Cris John Rubesh RajanDaniel JohnsonChristopher JonesThomas Peter JonesSalil JoshiBeat JostJuan Jose Juan CastellaNathan JurikIzabela JuszczakDimitrios KaminarisSergii KandybeiMichael James KaneYouen KangChandiprasad KarMatthias KaracsonDmitrii KarpenkovAnni KauniskangasJacob William KautzMichal Krzysztof KazaneckiFloris KeizerMatthew KenzieTjeerd 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MarconiEdoardo MarianiSaverio MarianiCarla Marin BenitoJörg MarksAlexander Mclean MarshallLucas MartelGabriele MartelliGiuseppe MartellottiLoris MartinazzoliMaurizio MartinelliDaniel Guillermo Martinez GomezDiego Martinez SantosFernando Martinez VidalAlexia Martorell GranollersAndré MassafferriRosen MatevAbhijit MathadViacheslav MatiuninClara MatteuzziKara Renee MattioliAndrea MauriEmilie MauriceJoan MauricioPierre Paul Louis MayencourtJose Mazorra de CosMichal MazurekMichael MccannLucas McconnellTamaki Holly McgrathNiall Thomas MchughAndrew McnabRonan McnultyBrian MeadowsGerwin MeierDmytro MelnychukFanjie MengMarcel MerkAndrea MerliLucas Meyer GarciaDexing MiaoHan MiaoMikhail MikhasenkoDiego Alejandro MilanesAlessandro MinottiElisa MinucciTristan MirallesBiljana MitreskaDominik Stefan MitzelAtanu ModakRizwaan Adeeb MohammedRazvan-Daniel MoiseSergei MokhnenkoEsteban Felipe Molina CardenasTitus MombächerMatthew David MonkStephane MonteilAngel Morcillo GomezGianfranco MorelloMichael 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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 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 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 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 Physical Review Letters le 02/11/2020

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Résumé : The $C\!P$ asymmetry and branching fraction of the CKM-suppressed decay $B^+\!\to J\mskip -3mu/\mskip -2mu\psi\,\pi^+$ are precisely measured relative to the favoured decay $B^+\!\to J\mskip -3mu/\mskip -2mu\psi\,K^+$, using a sample of proton-proton collision data corresponding to an integrated luminosity of $5.4~\mathrm{fb}^{-1}$ recorded at center-of-mass energy of $13~\mathrm{TeV}$ during 2016--2018. The results of the $C\!P$ asymmetry difference and branching fraction ratio are \begin{align*} \Delta\mathcal{A}^{C\!P} &\equiv \mathcal{A}^{C\!P}(B^+ \to J\mskip -3mu/\mskip -2mu\psi\,\pi^+) - \mathcal{A}^{C\!P}(B^+ \to J\mskip -3mu/\mskip -2mu\psi\,K^+) = (1.29 \pm 0.49 \pm 0.08) \times 10^{-2}, \end{align*}\begin{equation*} \mathcal{R}_{\pi/K} \equiv \frac{\mathcal{B}(B^+ \!\to J\mskip -3mu/\mskip -2mu\psi\,\pi^+)}{\mathcal{B}(B^+ \!\to J\mskip -3mu/\mskip -2mu\psi\,K^+)} = (3.852 \pm 0.022 \pm 0.018) \times 10^{-2}. \end{equation*} where the first uncertainties are statistical and the second systematic. A combination with previous LHCb results based on data collected at $7$ and $8~\mathrm{TeV}$ in 2011 and 2012 yields $\Delta\mathcal{A}^{C\!P} = (1.42 \pm 0.43 \pm 0.08) \times 10^{-2}$ and $\mathcal{R}_{\pi/K} = (3.846 \pm 0.018 \pm 0.018) \times 10^{-2}$. The combined $\Delta\mathcal{A}^{C\!P}$ value deviates from zero by 3.2 standard deviations, providing the first evidence for direct $C\!P$ violation in the amplitudes of beauty decays to charmonium final states.

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2025
• Auteurs : Bowei CaiMariana Tiscareno-AndradeYanru LuoFei CaoAurélie ChambonXinjie YuanMarion PeuchYashi ZhangAurélie HurelJulie GuérinNathalie VrielynckChristine MézardPhilippe AndreyLaurence CromerChao YangMathilde GrelonSandrine Lefranc
• Organismes : Institut Jean-Pierre Bourgin - Sciences du végétal Institut Jean-Pierre Bourgin - Sciences du végétal Institut Jean-Pierre Bourgin - Sciences du végétal Institut Jean-Pierre Bourgin - Sciences du végétal Institut Jean-Pierre Bourgin - Sciences du végétal Institut Jean-Pierre Bourgin - Sciences du végétal Institut Jean-Pierre Bourgin - Sciences du végétal Institut Jean-Pierre Bourgin - Sciences du végétal Institut Jean-Pierre Bourgin - Sciences du végétal Institut Jean-Pierre Bourgin - Sciences du végétal
• Publié dans Nature Plants le 21/10/2020

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Résumé : Homologous pairing and recombination during meiosis are facilitated by Rapid Prophase Movements (RPMs), which depend on chromosome attachment to the nuclear envelope (NE) and on cytoplasmic forces transmitted to the chromosomes through the NE, mediated by LINC (Linker of Nucleoskeleton and Cytoskeleton) complexes. In plants, only the NE-associated SUN domain proteins SUN1 and SUN2 have been identified as components of the RPM process. Here, we show that, during meiosis, SUN1 and SUN2 form a LINC complex with the KASH domain protein SINE3, which recruits the meiotic-specific kinesin PSS1 to the NE. These proteins accumulate at telomere-binding sites in the NE, and their loss disrupts telomere attachment, bouquet formation, and abolishes RPMs. These defects lead to defective synapsis and clustered crossovers, resulting in chromosome misegregation. Our results establish that the mechanism underlying RPMs is conserved in A. thaliana, with RPMs primarily facilitating homologous recognition rather than preventing non-homologous interactions.

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Fichiers liés : 20557_2_merged_1747204282.pdf

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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 AbramowiczHenso AbreuYiming AbulaitiBobby Samir AcharyaAnke AckermannClaire Adam BourdariosLeszek AdamczykSagar AddepalliMatt AddisonJahred AdelmanAytul AdiguzelTim AdyeTony AffolderYoav AfikMerve Nazlim AgarasJinky AgarwalaAnamika AggarwalCatalin AgheorghieseiAmmara AhmadFaig AhmadovWaleed Syed AhmedSudha AhujaXiaocong AiGiulio AielliArya AikotMalak Ait TamlihatBrahim AitbenchikhMelike AkbiyikTorsten AkessonAndrei AkimovDaiya AkiyamaNilima Nilesh AkolkarSina AktasKonie Al KhouryGian Luigi AlberghiJustin AlbertPietro AlbicoccoGuillaume AlbouySara AlderweireldtZackary Lee AlegriaMartin AleksaIgor AlexandrovCalin AlexaTheodoros AlexopoulosFabrizio AlfonsiMalte AlgrenMuhammad AlhroobBabar AliHanadi AliShahzad AliSamuel William AlibocusMalik AlievGianluca AlimontiWael AlkakhiCorentin AllaireBenedict AllbrookeJulia Frances AllenCristian Andres Allendes FloresPhilip Patrick AllportAlberto AloisioFrancisco AlonsoCristiano AlpigianiZainab Mohammad K AlsolamiManuel Alvarez EstevezAdrian Alvarez FernandezMario Alves CardosoMariagrazia AlviggiMohamed AlyYara Do Amaral CoutinhoAlessandro AmblerChristoph AmelungMaximilian AmerlChristoph AmesDante AmideiKyle AmirieSusana Patricia Amor dos SantosKieran Robert AmosShiwen AnViktor AnanievChristos AnastopoulosTimothy Robert AndeenJohn Kenneth AndersStefio Yosse AndreanAttilio AndreazzaStylianos AngelidakisAaron AngeramiAlexey AnisenkovAlberto AnnoviClaire AntelEgor AntipovMario AntonelliFabio AnulliMasato AokiTakumi AokiMarco AparoLudovica Aperio BellaChristian AppeltAram ApyanSergio Javier Arbiol ValChiara ArcangelettiAyana Tamu ArceEloisa ArenaJean-Francois ArguinSpyros ArgyropoulosJan-Hendrik ArlingOlivier ArnaezHannah ArnoldGiacomo ArtoniHaruka AsadaKanae AsaiShoji AsaiNedaa Alexandra AsbahRachel Amy Ashby PickeringKetevi Adikle AssamaganRobert AstalosKarl Sten Vilhelm 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• Organismes : Centre de Physique des Particules de Marseille Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire d'Annecy de Physique des Particules 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 des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules AstroParticule et Cosmologie Centre de Physique des Particules de Marseille AstroParticule et Cosmologie Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire d'Annecy de Physique des Particules 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 Laboratoire de Physique de Clermont Laboratoire de Physique de Clermont 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 d'Annecy de Physique des Particules 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 Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique Nucléaire et de Hautes Énergies 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 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 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 Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Centre de Physique des Particules de Marseille 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 Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique des 2 Infinis Irène Joliot-Curie 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 Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers 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 de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique 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Joliot-Curie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Institut de Recherches sur les lois Fondamentales de l'Univers Centre de Physique des Particules de Marseille Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille AstroParticule et Cosmologie Institut de Recherches sur les lois Fondamentales de l'Univers 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 de Clermont Centre de Physique des Particules de Marseille Institut de Recherches sur les lois Fondamentales de l'Univers 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 des deux Infinis de Toulouse 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 AstroParticule et Cosmologie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont 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 Centre de Physique des Particules de Marseille Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire des deux Infinis de Toulouse Centre de Physique des Particules de Marseille Laboratoire des deux Infinis de Toulouse Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Subatomique et de Cosmologie Laboratoire des deux Infinis de Toulouse Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Institut de Recherches sur les lois Fondamentales de l'Univers 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 : The Lund jet plane (LJP) is measured for the first time in $t\overline{t}$ events, using 140 fb$^{-1}$ of $\sqrt{s}$ = 13 TeV pp collision data collected with the ATLAS detector at the LHC. The LJP is a two-dimensional observable of the sub-structure of hadronic jets that acts as a proxy for the kinematics of parton showers and hadron formation. The observable is constructed from charged particles and is measured for R = 1.0 anti-$k_t$ jets with transverse momentum above 350 GeV containing the full decay products of either a top quark or a daughter $W$ boson. The other top quark in the event is identified from its decay into a b-quark, an electron or a muon and a neutrino. The measurement is corrected for detector effects and compared with a range of Monte Carlo predictions sensitive to different aspects of the hadronic decays of the heavy particles. In the $W$-boson-initiated jets, all the predictions are incompatible with the measurement. In the top quark initiated jets, disagreement with all predictions is observed in smaller subregions of the plane, and with a subset of the predictions across the fiducial plane. The measurement could be used to improve the tuning of Monte Carlo generators, for better modelling of hadronic decays of heavy quarks and bosons, or to improve the performance of jet taggers.

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