Diego SANCHEZ

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2018
• Auteurs : Roel AaijBernardo AdevaMarco AdinolfiZiad AjaltouniSimon AkarJohannes AlbrechtFederico AlessioMichael AlexanderAlejandro Alfonso AlberoSuvayu AliGeorgy AlkhazovPaula Alvarez CartelleAntonio Augusto AlvesSandra AmatoSilvia AmerioYasmine AmhisLiupan AnLucio AnderliniGuido AndreassiMirco AndreottiJason AndrewsRobert ApplebyFlavio ArchilliPhilippe d'ArgentJoan Arnau RomeuAlexander ArtamonovMarina ArtusoElie AslanidesGiulio AuriemmaMarouen BaalouchIgor BabuschkinSebastian BachmannJohn BackAlexey BadalovClarissa BaessoSophie BakerVladislav BalaguraWander BaldiniAlexander BaranovRoger BarlowColin BarschelSergey BarsukWilliam BarterFedor BaryshnikovVarvara BatozskayaVincenzo BattistaAurelio BayLeo BeaucourtJohn BeddowFranco BedeschiIgnacio BediagaAndrew BeiterLennaert BelNikita BeliyViolaine BelleeNicoletta BelloliKonstantin BelousIvan BelyaevEli Ben-HaimGiovanni BencivenniSean BensonSarah BeranekAlexander BerezhnoyRoland BernetDaniel BerninghoffEmilie BertholetAlessandro BertolinChristopher BetancourtFederico BettiMarc-Olivier BettlerMartinus van BeuzekomIaroslava BezshyikoSimone BifaniPierre BilloirAlex BirnkrautAlexander BitadzeAndrea BizzetiMikkel BjørnThomas BlakeFrederic BlancJohan BlouwSteven BluskValerio BocciThomas BoettcherAlexander BondarNikolay BondarWalter BoniventoIgor BordyuzhinAlessio BorgheresiSilvia BorghiMaxim BorisyakMartino BorsatoFrancesco BossuMeriem BoubdirThemistocles BowcockEspen Eie BowenConcezio BozziSvende BraunThomas BrittonJolanta BrodzickaDavide BrunduEmma BuchananChristopher BurrAlbert BurscheJan BuytaertWiktor ByczynskiSandro CadedduHao CaiRoberto CalabreseRyan CalladineMarta CalviMiriam Calvo GomezAlessandro CamboniPierluigi CampanaDaniel Hugo Campora PerezLorenzo CapriottiAngelo CarboneGiovanni CarboniRoberta CardinaleAlessandro CardiniPaolo CarnitiLaurence CarsonKazuyoshi Carvalho AkibaGianluigi CasseLorenzo CassinaLucia Castillo GarciaMarco CattaneoGiovanni CavalleroRiccardo CenciDavid ChamontMatthew George ChapmanMatthew CharlesPh. 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• Organismes : Laboratoire de Physique de Clermont Laboratoire de l'Accélérateur Linéaire Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille Laboratoire de Physique de Clermont Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire Laboratoire d'Annecy de Physique des Particules 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 l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire 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 d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique de Clermont Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de l'Accélérateur Linéaire 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 de Clermont Laboratoire de Physique de Clermont Centre de Physique des Particules de Marseille Laboratoire de l'Accélérateur Linéaire Laboratoire de Physique de Clermont Centre de Physique des Particules de Marseille Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire Centre de Physique des Particules de Marseille Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Centre de Physique des Particules de Marseille Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire 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 de Clermont Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de l'Accélérateur Linéaire Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de l'Accélérateur Linéaire Laboratoire de Physique Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille Laboratoire d'Annecy de Physique des Particules Centre de Physique des Particules de Marseille Laboratoire d'Annecy de Physique des Particules Laboratoire d'Annecy de Physique des Particules Centre de Physique des Particules de Marseille Laboratoire de l'Accélérateur Linéaire Laboratoire de Physique de Clermont Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire Laboratoire de l'Accélérateur Linéaire Laboratoire d'Annecy de Physique des Particules Laboratoire de l'Accélérateur Linéaire
• Publié dans Journal of High Energy Physics le 23/10/2020

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Résumé : The ratios of the branching fractions of the decays Λ$_{c}^{+}$ → pπ$^{−}$π$^{+}$, Λ$_{c}^{+}$ → pK$^{−}$K$^{+}$, and Λ$_{c}^{+}$ → pπ$^{−}$K$^{+}$ with respect to the Cabibbo-favoured Λ$_{c}^{+}$ → pK$^{−}$π$^{+}$ decay are measured using proton-proton collision data collected with the LHCb experiment at a 7 TeV centre-of-mass energy and corresponding to an integrated luminosity of 1.0 fb$^{−1}$: $ \begin{array}{l}\frac{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{\pi}^{-}{\pi}^{+}\right)}{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{\pi}^{+}\right)}=\left(7.44\pm 0.08\pm 0.18\right)\%,\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{K}^{+}\right)}{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{\pi}^{+}\right)}=\left(1.70\pm 0.03\pm 0.03\right)\%\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{\pi}^{-}{K}^{+}\right)}{\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{\pi}^{+}\right)}=\left(0.165\pm 0.015\pm 0.005\right)\%,\hfill \end{array} $ where the uncertainties are statistical and systematic, respectively. These results are the most precise measurements of these quantities to date. When multiplied by the world-average value for $ \mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{\pi}^{+}\right) $ , the corresponding branching fractions are $ \begin{array}{l}\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{\pi}^{-}{\pi}^{+}\right)=\left(4.72\pm 0.05\pm 0.11\pm 0.25\right)\times {10}^{-3},\hfill \\ {}\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{K}^{+}\right)=\left(1.08\pm 0.02\pm 0.02\pm 0.06\right)\times {10}^{-3},\hfill \\ {}\mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{\pi}^{-}{K}^{+}\right)=\left(1.04\pm 0.09\pm 0.03\pm 0.05\right)\times {10}^{-4},\hfill \end{array} $ where the final uncertainty is due to $ \mathrm{\mathcal{B}}\left({\varLambda}_c^{+}\to p{K}^{-}{\pi}^{+}\right) $ .

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Fichiers liés : 1711.01157.pdf

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2018
• Auteurs : Albert M SirunyanArmen TumasyanWolfgang AdamFederico AmbrogiEce AsilarThomas BergauerJohannes BrandstetterMarko DragicevicJanos EröAlberto Escalante del ValleMartin FlechlRudolf FruehwirthVasile Mihai GheteJosef HrubecManfred JeitlerNatascha KrammerIlse KrätschmerDietrich LikoThomas MadlenerIvan MikulecNavid RadHerbert RohringerJochen SchieckRobert SchöfbeckMarkus SpanringDaniel SpitzbartAnton TaurokWolfgang WaltenbergerJohannes WittmannClaudia-Elisabeth WulzMateusz ZaruckiVladimir ChekhovskyVladimir MossolovJuan Suarez GonzalezEddi A de WolfDavide Di CroceXavier JanssenJasper LauwersMaxim PietersMerijn van de KlundertHans van HaevermaetPierre van MechelenNick van RemortelShimaa Abu ZeidFreya BlekmanJorgen d'HondtIsabelle de BruynJarne de ClercqKevin DerooverGiannis FlourisDenys LontkovskyiSteven LowetteIvan MarchesiniSeth MoortgatLieselotte MoreelsQuentin PythonKirill SkovpenStefaan TavernierWalter van DoninckPetra van MuldersIsis van ParijsDiego BeghinBugra BilinHugues BrunBarbara ClerbauxGilles de LentdeckerHugo DelannoyBrian DorneyGiuseppe FasanellaLaurent FavartReza GoldouzianAnastasia GrebenyukAmandeep Kaur KalsiThomas LenziJelena LueticNicolas PostiauElizabeth StarlingLaurent ThomasCatherine Vander VeldePascal VanlaerDavid VanneromQun WangTom CornelisDidar DoburAlexis FagotMuhammad GulIllia KhvastunovDeniz PoyrazChristos RoskasDaniele TrocinoMichael TytgatWillem VerbekeBasile VermassenMartina VitNicolas ZaganidisHamed BakhshiansohiOlivier BonduSébastien BrochetGiacomo BrunoClaudio CaputoPieter DavidChristophe DelaereMartin DelcourtBrieuc FrancoisAndrea GiammancoGeorgios KrintirasVincent LemaitreAlessio MagitteriAlexandre MertensMarco MusichKrzysztof PiotrzkowskiAlessia SaggioMiguel Vidal MaronoSébastien WertzJoze ZobecFábio Lúcio AlvesGilvan AlvesLucas BritoMarcos Correa MartinsGilson Correia SilvaCarsten HenselArthur MoraesMaria Elena PolPatricia Rebello TelesEwerton Belchior Batista das ChagasWagner CarvalhoJose ChinellatoEduardo CoelhoEliza 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LindénPanja-Riina LuukkaTeppo MäenpääHannu SiikonenEija TuominenJorma TuominiemiTuure TuuvaMarc BesanconFabrice CoudercMarc DejardinDaniel DenegriJean-Louis FaureFederico FerriSerguei GanjourAlain GivernaudPhilippe GrasGautier Hamel de MonchenaultPatrick JarryClément LeloupElizabeth LocciJulie MalclesGiulia NegroJohn RanderAndré RosowskyMehmet Özgür SahinMaksym TitovAbdulla AbdulsalamChiara AmendolaIurii AntropovFlorian BeaudettePhilippe BussonClaude CharlotRaphael Granier de CassagnacInna KucherStanislav LisniakArtur LobanovJavier Martin BlancoMatthew NguyenChristophe OchandoGiacomo OrtonaPhilipp PigardRoberto SalernoJean-Baptiste SauvanYves SiroisAndre Govinda Stahl LeitonAlexandre ZabiAmina ZghicheJean-Laurent AgramJeremy AndreaDaniel BlochJean-Marie BromEric Christian ChabertVladimir CherepanovCaroline CollardEric ConteJean-Charles FontaineDenis GeléUlrich GoerlachMarkéta JansováAnne-Catherine Le BihanNicolas TononPierre van HoveSébastien GadratStephanie BeauceronColin BernetGaelle 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• Publié dans Journal of High Energy Physics le 23/10/2020

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Résumé : A search in energetic, high-multiplicity final states for evidence of physics beyond the standard model, such as black holes, string balls, and electroweak sphalerons, is presented. The data sample corresponds to an integrated luminosity of 35.9 fb$^{−1}$ collected with the CMS experiment at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV in 2016. Standard model backgrounds, dominated by multijet production, are determined from control regions in data without any reliance on simulation. No evidence for excesses above the predicted background is observed. Model-independent 95% confidence level upper limits on the cross section of beyond the standard model signals in these final states are set and further interpreted in terms of limits on semiclassical black hole, string ball, and sphaleron production. In the context of models with large extra dimensions, semiclassical black holes with minimum masses as high as 10.1 TeV and string balls with masses as high as 9.5 TeV are excluded by this search. Results of the first dedicated search for electroweak sphalerons are presented. An upper limit of 0.021 is set at 95% confidence level on the fraction of all quark-quark interactions above the nominal threshold energy of 9 TeV resulting in the sphaleron transition.

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