Diego SANCHEZ

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2021
• Auteurs : Albert M SirunyanArmen TumasyanWolfgang AdamFederico AmbrogiThomas BergauerMarko DragicevicJanos EröAlberto Escalante del ValleRudolf FruehwirthManfred JeitlerNatascha KrammerLukas LechnerDietrich LikoThomas MadlenerIvan MikulecFlorian Michael PittersNavid RadJochen SchieckRobert SchöfbeckMarkus SpanringSebastian TemplWolfgang WaltenbergerClaudia-Elisabeth WulzMateusz ZaruckiVladimir ChekhovskyAliaksandr LitominVladimir MakarenkoJuan Suarez GonzalezMohamed Rashad DarwishEddi A de WolfDavide Di CroceXavier JanssenTomas KelloAleksandra LelekMaxim PietersHaifa Rejeb SfarHans van HaevermaetPierre van MechelenSenne van PutteNick van RemortelFreya BlekmanEmil Sørensen BolsSimranjit Singh ChhibraJorgen d'HondtJarne de ClercqDenys LontkovskyiSteven LowetteIvan MarchesiniSeth MoortgatAlexander MortonQuentin PythonStefaan TavernierWalter van DoninckPetra van MuldersDiego BeghinBugra BilinBarbara ClerbauxGilles de LentdeckerBrian DorneyLaurent FavartAnastasia GrebenyukAmandeep Kaur KalsiInna MakarenkoLouis MoureauxLaurent PétréAndrey PopovNicolas PostiauElizabeth StarlingLaurent ThomasCatherine Vander VeldePascal VanlaerDavid VanneromLiam WezenbeekTom CornelisDidar DoburMarek GruchalaIllia KhvastunovMarek NiedzielaChristos RoskasKirill SkovpenMichael TytgatWillem VerbekeBasile VermassenMartina VitGiacomo BrunoFlorian Joel J BuryClaudio CaputoPieter DavidChristophe DelaereMartin DelcourtIzzeddin Suat DonertasAndrea GiammancoVincent LemaitreKuntal MondalJessica PrisciandaroAngela TaliercioMaksym TeklishynPietro VischiaSophie WuyckensJoze ZobecGilvan AlvesGilson Correia SilvaCarsten HenselArthur MoraesWalter Luiz Aldá JúniorEwerton Belchior Batista das ChagasHelena Brandao MalbouissonWagner CarvalhoJose ChinellatoEduardo CoelhoEliza Melo da CostaGustavo Gil da SilveiraDilson de Jesus DamiaoSandro Fonseca de SouzaJordan MartinsDiego Matos FigueiredoMiguel Medina JaimeMiqueias Melo de AlmeidaClemencia Mora HerreraLuiz MundimHelio NogimaPatricia Rebello TelesLuis Sanchez RosasAlberto SantoroSheila Mara Silva Do AmaralAndre SznajderMauricio ThielEdmilson José Tonelli ManganoteFelipe Torres da Silva de AraujoAntonio Vilela PereiraCesar Augusto BernardesLuigi CalligarisThiago TomeiEduardo de Moraes GregoresDener de Souza LemosPedro G MercadanteSergio F NovaesSandra PadulaAleksandar AleksandrovGeorgy AntchevIvan AtanasovRoumyana HadjiiskaPlamen IaydjievMilena MishevaMircho RodozovMariana ShopovaGeorgi SultanovMiroslav BonchevAnton DimitrovTodor IvanovLeander LitovBorislav PavlovPeicho PetkovAnton PetrovWenxing FangQianying GuoHanwen WangLi YuanMuhammad AhmadZhen HuYi WangEmilien ChaponGuo-Ming ChenHe-Sheng ChenMingshui ChenAnshul KapoorDuncan LeggatHongbo LiaoZhenan LiuRamkrishna SharmaAniello SpieziaJunquan TaoJoshuha Thomas-WilskerJin WangHuaqiao ZhangSijing ZhangJingzhou ZhaoAntonis AgapitosYong BanCheng ChenAndrew LevinQiang LiMeng LuXudong LyuYajun MaoSi-Jin QianDayong WangQun WangJie XiaoZhengyun YouXuyang GaoMeng XiaoCarlos AvilaAndrés CabreraCarlos FlorezJorge FragaAmal SarkarManuel Alejandro Segura DelgadoJohny JaramilloJhovanny Mejia GuisaoFelipe RamirezJosé David Ruiz AlvarezCamilo Andrés Salazar GonzálezNelson Vanegas ArbelaezDuje GiljanovicNikola GodinovicDamir LelasIvica PuljakToni SculacZeljko AntunovicMarko KovacVuko BrigljevicDinko FerencekDevdatta MajumderMatej RoguljicAndrei StarodumovTatjana SusaMohsan Waseem AtherAlexandros AttikisEleni ErodotouAimilios IoannouGouranga KoleMarina KolosovaSotiroulla KonstantinouGeorgios MavromanolakisJehad MousaCharalambos NicolaouFotios PtochosPanos A RazisHans RykaczewskiHalil SakaDemetra TsiakkouriMiroslav FingerMichael FingerAntonin KvetonJan TomsaEdy AyalaEdgar Carrera JarrinAhmed Ali AbdelalimSherif ElgammalAli Ellithi KamelMohammed MahmoudYasser MohammedSandeep BhowmikAlexandra Carvalho Antunes de OliveiraRam Krishna DewanjeeKarl EhatahtMario KadastikMartti RaidalChristian VeelkenPaula EerolaLaurent ForthommeHenning KirschenmannKenneth OsterbergMikko 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• Publié dans JHEP le 17/11/2025

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Résumé : Measurements of the differential cross sections of Z + jets and γ + jets production, and their ratio, are presented as a function of the boson transverse momentum. Measurements are also presented of the angular distribution between the Z boson and the closest jet. The analysis is based on pp collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 35.9 fb$^{−1}$ recorded by the CMS experiment at the LHC. The results, corrected for detector effects, are compared with various theoretical predictions. In general, the predictions at higher orders in perturbation theory show better agreement with the measurements. This work provides the first measurement of the ratio of the differential cross sections of Z + jets and γ + jets production at 13 TeV, as well as the first direct measurement of Z bosons emitted collinearly with a jet.[graphic not available: see fulltext]

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2021
• Auteurs : Roel AaijCarlos Abellán BetetaThomas AckernleyBernardo AdevaMarco AdinolfiHossein AfsharniaChristine Angela AidalaSalvatore AiolaZiad AjaltouniSimon AkarJohannes AlbrechtFederico AlessioMichael AlexanderAlejandro Alfonso AlberoZakariya AlioucheGeorgy AlkhazovPaula Alvarez CartelleSandra AmatoYasmine AmhisLiupan AnLucio AnderliniAleksei AndreianovMirco AndreottiFlavio ArchilliAlexander ArtamonovMarina ArtusoKenenbek ArzymatovElie AslanidesMichele AtzeniBenjamin AudurierSebastian BachmannMarie BachmayerJohn BackPablo Baladron RodriguezVladislav BalaguraWander BaldiniJuan Baptista LeiteRoger BarlowSergey BarsukWilliam BarterMatteo BartoliniFedor BaryshnikovJan-Marc BaselsGiovanni BassiBaasansuren BatsukhAlexander BattigAurelio BayMaik BeckerFranco BedeschiIgnacio BediagaAndrew BeiterVladislav BelavinSamuel BelinViolaine BelleeKonstantin BelousIlia BelovIvan BelyaevGiovanni BencivenniEli Ben-HaimAlexander BerezhnoyRoland BernetDaniel BerninghoffHarris Conan BernsteinClaudia BertellaAlessandro BertolinChristopher BetancourtFederico BettiIaroslava BezshyikoSrishti BhasinJihyun BhomLingzhu BianMartin Stefan BiekerSimone BifaniPierre BilloirMatthew BirchFionn Caitlin Ros BishopAlexander BitadzeAndrea BizzetiMikkel BjørnMichele Piero BlagoThomas BlakeFrederic BlancSteven BluskDana BobulskaJulian Alexander BoelhauveOscar Boente GarciaThomas BoettcherAlexey BoldyrevAlexander BondarNikolay BondarSilvia BorghiMaxim BorisyakMartino BorsatoJozef Tomasz BorsukSonia Amina BouchibaThemistocles BowcockAlexandre BoyerConcezio BozziMatthew John BradleySvende BraunAlexandre Brea RodriguezMichael BrodskiJolanta BrodzickaArnau Brossa GonzaloDavide BrunduAnnarita BuonauraChristopher BurrAlbert BurscheAnatoly ButkevichJordy Sebastiaan ButterJan BuytaertWiktor ByczynskiSandro CadedduHao CaiRoberto CalabreseLukas CaleficeLiliet Calero DiazStefano CaliRyan CalladineMarta CalviMiriam Calvo GomezPatricia Camargo MagalhaesAlessandro CamboniPierluigi CampanaAngel Fernando Campoverde QuezadaSimone CapelliLorenzo CapriottiAngelo CarboneGiovanni CarboniRoberta CardinaleAlessandro CardiniIna CarliPaolo CarnitiLeon David CarusKazuyoshi Carvalho AkibaAdrian Casais VidalGianluigi CasseMarco CattaneoGiovanni CavalleroSara CelaniJacopo CerasoliAbbie Jane ChadwickMatthew George ChapmanMatthew CharlesPh. CharpentierGeorgios ChatzikonstantinidisCarlos Alberto Chavez BarajasMaximilien ChefdevilleChen ChenShanzhen ChenAleksei ChernovVeronika ChobanovaSerhii CholakMarcin ChrzaszczAlexsei ChubykinVladimir ChulikovPaolo CiambroneMaria Flavia CicalaXabier Cid VidalGregory CiezarekPeter ClarkeMarco ClemencicHarry CliffJoel ClosierJohn Leslie CobbledickVictor CocoJoao a B CoelhoJulien CoganEric CognerasLucian CojocariuPaula CollinsTommaso ColomboLiliana CongedoAndrea ContuNaomi CookeGeorge CoombsGloria CortiCayo Mar Costa SobralBenjamin CouturierDaniel Charles CraikJana CrkovskáMelissa Maria Cruz TorresRobert CurrieCesar Luiz da SilvaElena Dall'OccoJeremy DalsenoCarmelo d'AmbrosioAnna DanilinaPhilippe d'ArgentAdam DavisOscar de Aguiar FranciscoKristof de BruynStefano de CapuaMichel de CianJussara de MirandaLeandro de PaulaMarilisa de SerioDario de SimonePatrizia de SimoneJacco de VriesCameron Thomas DeanDaniel DecampLuigi del BuonoBlaise DelaneyHans Peter DembinskiAdam DendekVadym DenysenkoDenis DerkachOlivier DeschampsFabrice DesseFrancesco DettoriBiplab DeyPasquale Di NezzaSergey DidenkoLorena Dieste MaronasHans DijkstraVasyl DobishukAmanda May DonohoeFrancesca DordeiAlberto dos ReisLauren DouglasAnatoliy DovbnyaAnthony Gavin DownesKarlis DreimanisMaciej Wojciech DudekLaurent DufourViacheslav DukPaolo DuranteJohn Matthew DurhamDeepanwita DuttaAgnieszka DziurdaAlexey DzyubaSajan EasoUlrik EgedeVictor EgorychevSemen EidelmanStephan EisenhardtSurapat Ek-InLars EklundScott ElyAlexandru EneEliane EppleStephan EscherJonas Nathanael EschleSevda EsenTimothy EvansAntonio FalabellaJingzhou FanYanting FanBo FangStephen FarryDavide FazziniMauricio FéoAntonio Fernandez PrietoJose Maria Fernandez-Tenllado ArribasFabio FerrariLino Ferreira LopesFernando Ferreira RodriguesSilvia Ferreres SoleMartina FerrilloMassimiliano Ferro-LuzziSergey FilippovRosa Anna FiniMassimiliano FioriniMiroslaw FirlejKamil Leszek FischerConor FitzpatrickTomasz FiutowskiFrederic FleuretMarianna FontanaFlavio FontanelliRoger FortyVinicius Franco LimaManuel Franco SevillaMarkus FrankEdoardo FranzosoGiulia FrauChristoph FreiDavid Anthony FridayJinlin FuQuentin FuehringWolfgang FunkEmmy GabrielTatiana GaintsevaAbraham Gallas TorreiraDomenico GalliSilvia GambettaYuyue GanMiriam GandelmanPaolo GandiniYuanning GaoMichela GarauLuis Miguel Garcia MartinPaula Garcia MorenoJulián García PardiñasBeatriz Garcia PlanaFelipe Andres Garcia RosalesLluis GarridoClara GasparRobbert Erik GeertsemaDavid GerickLouis Lenard GerkenEvelina GersabeckMarco GersabeckTimothy GershonDawid GerstelPhilippe GhezValerie GibsonHenryk Karol GiemzaMatteo GiovannettiAlessandra GioventùPere Gironella GironellLavinia-Helena GiubegaCarmen GiuglianoKonstantin GizdovEvangelos Leonidas GkougkousisVladimir GligorovCarla GöbelElisabet GolobardesDmitry GolubkovAndrey GolutvinAlvaro GomesSergio Gomez FernandezFernanda Goncalves AbrantesMateusz GoncerzGuanghua GongPetr GorbounovIgor Vladimirovich GorelovClaudio GottiEkaterina GovorkovaJascha Peter GrabowskiThomas GrammaticoLuis Alberto Granado CardosoEugeni GraugésElena GraveriniGiacomo GrazianiAlexandru GrecuLex Marinus GreevenPeter GriffithLucia GrilloSergey GromovBarak Raimond Gruberg CazonChenxi GuMarco GuarisePaul Andre GüntherEvgeny GushchinAndreas GuthYury GuzThierry GysThomas HadavizadehGuido HaefeliT. 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ShieldsEvgenii ShmaninJoseph David ShupperdBenedetto Gianluca SiddiRafael Silva CoutinhoGabriele SimiSaverio SimoneNicola SkidmoreTomasz SkwarnickiMark SlaterIgor SlazykJennifer Clare SmallwoodJohn Gordon SmeatonAnastasia SmetkinaEluned SmithMark SmithAleksandra SnochMarcelo SoaresLais Soares LavraMichael SokoloffPaul SolerAleksandr SolovevIvan SolovyevFelipe Luan Souza de AlmeidaBruno Souza de PaulaBernhard SpaanElisabetta Spadaro NorellaPatrick SpradlinFederico StagniMarian StahlSascha StahlPavol StefkoOlaf SteinkampOleg StenyakinHolger StevensSheldon StoneMaria Elena StramagliaMihai StraticiucDaria StrekalinaFidan SuljikJiayin SunLiang SunYipeng SunPeter SvihraPaul Nathaniel SwallowKrzysztof SwientekAdam SzabelskiTomasz SzumlakMaciej Pawel SzymanskiShantam TanejaFrederic TeubertEric ThomasKayleigh Anne ThomsonVincent TisserandStephane t'JampensMark TobinLuca TomassettiDiego Torres Machadoda Yu TouMinh Tâm TranEkaterina TrifonovaCarina TripplGiulia TuciAlison TullyNiels TuningArtur 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Vilella FiguerasZhenzi WangZirui WangHeather Mckenzie WarkNigel WatsonSteffen Georg WeberDavid WebsdaleConstantin WeisserBenedict Donald C WesthenryDylan Jaide WhiteMark WhiteheadDirk WiednerGuy WilkinsonMichael WilkinsonIfan WilliamsMike WilliamsMark Richard James WilliamsFergus WilsonWojciech WislickiMariusz WitekLukas WitolaGuy WormserStephen WottonHangyi WuKenneth WyllieZhiyu XiangDong XiaoYuehong XieAo XuJingyi XuLi XuMenglin XuQingnian XuZehua XuZhihao XuDi YangShuangli YangYouhua YangZhenwei YangZishuo YangYuezhe YaoLauren Emma YeomansHang YinJiesheng YuXuhao YuanOleg YushchenkoEttore ZaffaroniMikhail ZavertyaevMilosz ZdybalOleksandr ZenaievMing ZengDongliang ZhangLiming ZhangShunan ZhangYanxi ZhangYu ZhangAlexey ZhelezovYangheng ZhengXiaokang ZhouYixiong ZhouXianglei ZhuValery ZhukovJennifer Brigitta ZonneveldQuan ZouStefano ZucchelliDavide ZulianiGianluca Zunica
• Organismes : 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 Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Centre de Physique des Particules de Marseille Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique de Clermont 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 de Physique Nucléaire et de Hautes Énergies Laboratoire Leprince-Ringuet Centre de Physique des Particules de Marseille Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille Laboratoire de Physique de Clermont 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 de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire Leprince-Ringuet Centre de Physique des Particules de Marseille Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique de Clermont Laboratoire de Physique des 2 Infinis Irène Joliot-Curie 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 Centre de Physique des Particules de Marseille Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules 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 Laboratoire de Physique de Clermont Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille Laboratoire de Physique Nucléaire et de Hautes Énergies 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 : The Cabibbo-suppressed decay $\Lambda_b^0\rightarrow\chi_{c1}p\pi^-$ is observed for the first time using data from proton-proton collisions corresponding to an integrated luminosity of 6fb$^{-1}$, collected with the LHCb detector at a centre-of-mass energy of 13TeV. Evidence for the $\Lambda_b^0\rightarrow\chi_{c2}p\pi^-$ decay is also found. Using the $\Lambda_b^0\rightarrow\chi_{c1}pK^-$ decay as normalisation channel, the ratios of branching fractions are measured to be $\begin{array}{rcl} \frac{ \mathcal{B} (\Lambda_b^0\rightarrow\chi_{c1}p\pi^-)}{\mathcal{B} (\Lambda_b^0\rightarrow\chi_{c1}pK^-)} & = & (6.59 \pm 1.01 \pm 0.22 ) \times 10^{-2} \,, \frac{\mathcal{B} (\Lambda_b^0\rightarrow\chi_{c2}p\pi^-)}{\mathcal{B} (\Lambda_b^0\rightarrow\chi_{c1}p\pi^-)} & = & 0.95 \pm 0.30 \pm 0.04 \pm 0.04 \,, \frac{\mathcal{B} (\Lambda_b^0\rightarrow\chi_{c2}pK^-)}{\mathcal{B} (\Lambda_b^0\rightarrow\chi_{c1}pK^-)} & = & 1.06 \pm 0.05 \pm 0.04 \pm 0.04 \,,\end{array}$ where the first uncertainty is statistical, the second is systematic and the third is due to the uncertainties in the branching fractions of $\chi_{c1,2}\rightarrow J/\psi\gamma$ decays.

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2021
• Auteurs : Roel AaijCarlos Abellán BetetaThomas AckernleyBernardo AdevaMarco AdinolfiHossein AfsharniaChristine Angela AidalaSalvatore AiolaZiad AjaltouniSimon AkarJohannes AlbrechtFederico AlessioMichael AlexanderAlejandro Alfonso AlberoZakariya AlioucheGeorgy AlkhazovPaula Alvarez CartelleSandra AmatoYasmine AmhisLiupan AnLucio AnderliniAleksei AndreianovMirco AndreottiFlavio ArchilliAlexander ArtamonovMarina ArtusoKenenbek ArzymatovElie AslanidesMichele AtzeniBenjamin AudurierSebastian BachmannMarie BachmayerJohn BackPablo Baladron RodriguezVladislav BalaguraWander BaldiniJuan Baptista LeiteRoger BarlowSergey BarsukWilliam BarterMatteo BartoliniFedor BaryshnikovJan-Marc BaselsGiovanni BassiBaasansuren BatsukhAlexander BattigAurelio BayMaik BeckerFranco BedeschiIgnacio BediagaAndrew BeiterVladislav BelavinSamuel BelinViolaine BelleeKonstantin BelousIlia BelovIvan BelyaevGiovanni BencivenniEli Ben-HaimAlexander BerezhnoyRoland BernetDaniel BerninghoffHarris Conan BernsteinClaudia BertellaAlessandro BertolinChristopher BetancourtFederico BettiIaroslava BezshyikoSrishti BhasinJihyun BhomLingzhu BianMartin Stefan BiekerSimone BifaniPierre BilloirMatthew BirchFionn Caitlin Ros BishopAlexander BitadzeAndrea BizzetiMikkel BjørnMichele Piero BlagoThomas BlakeFrederic BlancSteven BluskDana BobulskaJulian Alexander BoelhauveOscar Boente GarciaThomas BoettcherAlexey BoldyrevAlexander BondarNikolay BondarSilvia BorghiMaxim BorisyakMartino BorsatoJozef Tomasz BorsukSonia Amina BouchibaThemistocles BowcockAlexandre BoyerConcezio BozziMatthew John BradleySvende BraunAlexandre Brea RodriguezMichael BrodskiJolanta BrodzickaArnau Brossa GonzaloDavide BrunduAnnarita BuonauraChristopher BurrAlbert BurscheAnatoly ButkevichJordy Sebastiaan ButterJan BuytaertWiktor ByczynskiSandro CadedduHao CaiRoberto CalabreseLukas CaleficeLiliet Calero DiazStefano CaliRyan CalladineMarta CalviMiriam Calvo GomezPatricia Camargo MagalhaesAlessandro CamboniPierluigi CampanaAngel Fernando Campoverde QuezadaSimone CapelliLorenzo CapriottiAngelo CarboneGiovanni CarboniRoberta CardinaleAlessandro CardiniIna CarliPaolo CarnitiLeon David CarusKazuyoshi Carvalho AkibaAdrian Casais VidalGianluigi CasseMarco CattaneoGiovanni CavalleroSara CelaniJacopo CerasoliAbbie Jane ChadwickMatthew George ChapmanMatthew CharlesPh. CharpentierGeorgios ChatzikonstantinidisCarlos Alberto Chavez BarajasMaximilien ChefdevilleChen ChenShanzhen ChenAleksei ChernovVeronika ChobanovaSerhii CholakMarcin ChrzaszczAlexsei ChubykinVladimir ChulikovPaolo CiambroneMaria Flavia CicalaXabier Cid VidalGregory CiezarekP.E. L. 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• Organismes : 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 Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Centre de Physique des Particules de Marseille Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique de Clermont 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 de Physique Nucléaire et de Hautes Énergies Laboratoire Leprince-Ringuet Centre de Physique des Particules de Marseille Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille Laboratoire de Physique de Clermont 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 de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire Leprince-Ringuet Centre de Physique des Particules de Marseille Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique de Clermont Laboratoire de Physique des 2 Infinis Irène Joliot-Curie 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 Centre de Physique des Particules de Marseille Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules 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 de Clermont Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille Laboratoire de Physique Nucléaire et de Hautes Énergies 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 : The first full angular analysis of the $ {B}^0\to {D}^{\ast -}{D}_s^{\ast +} $ decay is performed using 6 fb$^{−1}$ of pp collision data collected with the LHCb experiment at a centre-of-mass energy of 13 TeV. The $ {D}_s^{\ast +}\to {D}_s^{+}\gamma $ and D$^{*−}$ → $ {\overline{D}}^0{\pi}^{-} $ vector meson decays are used with the subsequent $ {D}_s^{+} $ → K$^{+}$K$^{−}$π$^{+}$ and $ {\overline{D}}^0 $ → K$^{+}$π$^{−}$ decays. All helicity amplitudes and phases are measured, and the longitudinal polarisation fraction is determined to be f$_{L}$ = 0.578 ± 0.010 ± 0.011 with world-best precision, where the first uncertainty is statistical and the second is systematic. The pattern of helicity amplitude magnitudes is found to align with expectations from quark-helicity conservation in B decays. The ratio of branching fractions [ℬ($ {B}^0\to {D}^{\ast -}{D}_s^{\ast +} $) × ℬ($ {D}_s^{\ast +}\to {D}_s^{+}\gamma $)]/ℬ(B$^{0}$ → D$^{*−} {D}_s^{+} $) is measured to be 2.045 ± 0.022 ± 0.071 with world-best precision. In addition, the first observation of the Cabibbo-suppressed B$_{s}$ → D$^{*−} {D}_s^{+} $ decay is made with a significance of seven standard deviations. The branching fraction ratio ℬ(B$_{s}$ → D$^{*−} {D}_s^{+} $)/ℬ(B$^{0}$ → D$^{*−} {D}_s^{+} $) is measured to be 0.049 ± 0.006 ± 0.003 ± 0.002, where the third uncertainty is due to limited knowledge of the ratio of fragmentation fractions.[graphic not available: see fulltext]

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