Diego SANCHEZ

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2024
• 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 AgheorghieseiFaig 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 AmideiBaktash AminiKyle AmirieSusana Patricia Amor dos SantosKieran Robert AmosDimitra AmperiadouShiwen AnViktor AnanievChristos AnastopoulosTimothy Robert AndeenJohn Kenneth AndersAdam Campbell AndersonStefio Yosse AndreanAttilio AndreazzaStylianos AngelidakisAaron AngeramiAlexey AnisenkovAlberto AnnoviClaire AntelEgor AntipovMario AntonelliFabio AnulliMasato AokiTakumi AokiMarco AparoLudovica Aperio BellaChristian AppeltAram ApyanSergio Javier Arbiol ValChiara ArcangelettiAyana Tamu ArceJean-Francois ArguinSpyros ArgyropoulosJan-Hendrik ArlingOlivier ArnaezHannah ArnoldGiacomo ArtoniHaruka AsadaKanae AsaiShoji AsaiNedaa Alexandra AsbahRachel Amy Ashby PickeringKetevi Adikle AssamaganRobert AstalosKarl Sten Vilhelm AstrandRose AtashiRyan Justin AtkinMarkus Julian AtkinsonHicham AtmaniPrachi AtmasiddhaKamil AugstenSilvia AuricchioAdrien AuriolVolker Andreas AustrupGiuseppe AvolioKonstantinos AxiotisGeorges AzuelosDominik BabalHenri BachacouKonstantinos BachasAlexander BachiuKarl Filip BackmanAnthony BadeaTamas Marton BaerPaolo BagnaiaMarzieh BahmaniDaniel BahnerKehang BaiJohn BainesLuke BainesKeith BakerEvelin BakosDebottam Bakshi GuptaLuiz Eduardo Balabram FilhoVeena BalakrishnanRahul BalasubramanianEvgenii BaldinPetr BalekEric BallabeneFabrice BalliLisa Marie BaltesWilliam Keaton BalunasJohannes BalzIsaac BamwidhiElzbieta BanasMarilena BandieramonteAnjishnu BandyopadhyayShubham BansalLiron BarakMarawan BarakatElisabetta BarberioDario BarberisMarlon Benoit BarberoMarten Zefanja BarelTeresa BarillariMartin BarisitsTim BarklowPetr BaronDiego BaronToni BaroncelliAlan BarrJackson BarrBarreiro Barreiro AlonsoJoao Barreiro Guimaraes da CostaUriel BarronMaura BarrosSergey 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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 Laboratoire d'Annecy de Physique des Particules 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 Laboratoire de Physique Nucléaire et de Hautes Énergies 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 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 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 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 des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules 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 de Clermont Laboratoire de Physique Nucléaire et de Hautes Énergies 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 d'Annecy de Physique des Particules AstroParticule et Cosmologie Institut de Recherches sur les lois Fondamentales de l'Univers 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 Laboratoire de Physique de Clermont Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Subatomique et de Cosmologie Laboratoire des deux Infinis de Toulouse AstroParticule et Cosmologie Laboratoire de Physique des 2 Infinis Irène 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 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 JHEP le 17/11/2025

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Résumé : A search for neutral long-lived particles (LLPs) decaying in the ATLAS hadronic calorimeter using 140 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=13$ TeV delivered by the LHC is presented. The analysis is composed of three channels. The first targets pair-produced LLPs, where at least one LLP is produced with sufficiently low boost that its decay products can be resolved as separate jets. The second and third channels target LLPs respectively produced in association with a $W$ or $Z$ boson that decays leptonically. In each channel, different search regions target different kinematic regimes, to cover a broad range of LLP mass hypotheses and models. No excesses of events relative to the background predictions are observed. Higgs boson branching fractions to pairs of hadronically decaying neutral LLPs larger than 1% are excluded at 95% confidence level for proper decay lengths in the range of 30 cm to 4.5 m depending on the LLP mass, a factor of three improvement on previous searches in the hadronic calorimeter. The production of long-lived dark photons in association with a $Z$ boson with cross-sections above 0.1 pb is excluded for dark photon mean proper decay lengths in the range of 20 cm to 50 m, improving previous ATLAS results by an order of magnitude. Finally, long-lived photo-phobic axion-like particle models are probed for the first time by ATLAS, with production cross-sections above 0.1 pb excluded in the 0.1 mm to 10 m range.

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2024
• 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 AslanidesMichele AtzeniBenjamin AudurierDavid BacherIrene Bachiller PereaSebastian BachmannMarie BachmayerJohn BackPablo Baladron RodriguezVladislav BalaguraWander BaldiniJuan Baptista de Souza LeiteMatteo BarbettiIvanildo Rui BarbosaRoger BarlowSergey BarsukWilliam BarterMatteo BartoliniJustin BartzFedor BaryshnikovJan-Marc BaselsGiovanni BassiBaasansuren BatsukhAlexander BattigAurelio BayAnja BeckMaik BeckerFranco BedeschiIgnacio BediagaAndrew BeiterSamuel BelinViolaine BelleeKonstantin BelousIlia BelovIvan BelyaevGaya BenaneGiovanni BencivenniEli Ben-HaimAlexander BerezhnoyRoland BernetSergi Bernet AndresClaudia BertellaAlessandro 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 BolzonellaNikolay BondarFederica BorgatoSilvia BorghiMartino BorsatoJozef Tomasz BorsukSonia Amina BouchibaThemistocles BowcockAlexandre BoyerConcezio BozziMatthew John BradleyAlexandre Brea RodriguezNils BreerJolanta BrodzickaArnau Brossa GonzaloJames David BrownDavide BrunduEmma 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• Publié dans Physical Review D le 02/11/2020

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Résumé : The four decays, $\Lambda_{b}^{0} \rightarrow \Sigma_c^{(*)++} D^{(*)-} K^{-}$, are observed for the first time using proton-proton collision data collected with the LHCb detector at a centre-of-mass energy of $13\,\rm{TeV}$, corresponding to an integrated luminosity of $6\,\rm{fb}^{-1}$. By considering the $\Lambda_b^0 \rightarrow \Lambda_c^{+} \overline{D}^0 K^{-}$ decay as reference channel, the following branching fraction ratios are measured to be, $$\frac{\cal{B} (\Lambda_{b}^{0} \rightarrow \Sigma_{c}^{++} \rm{D}^{-} {K}^{-})}{\cal{B}(\Lambda_{b}^{0} \rightarrow \Lambda_c^{+} \rm \overline{D}^0 {K}^{-})} = {0.282}\pm{0.016}\pm{0.016}\pm{0.005}, \frac{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_{c}^{*++} \rm {D}^{-} {K}^{-})}{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_c^{++} \rm {D}^{-} {K}^{-})} = {0.460}\pm{0.052}\pm{0.028}, \frac{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_{c}^{++} \rm {D}^{*-} {K}^{-})}{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_c^{++} \rm {D}^{-} {K}^{-})} = {2.261}\pm{0.202}\pm{0.129}\pm{0.046}, \frac{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_{c}^{*++} \rm D^{*-} K^{-})}{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_c^{++} \rm D^{-} K^{-})} = {0.896}\pm{0.137}\pm{0.066}\pm{0.018},$$ where the first uncertainties are statistical, the second are systematic, and the third are due to uncertainties in the branching fractions of intermediate particle decays. These initial observations mark the beginning of pentaquark searches in these modes, with more data set to become available following the LHCb upgrade.

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