Carlos Moreno

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• Type de publi. : Ouvrage (y compris édition critique et traduction)
• Date de publi. : 07/06/2024
• Auteurs : Carlos Moreno
• Organismes : IAE Paris - Sorbonne Business School

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Résumé : In The 15-Minute City: A Solution for Saving Our Time and Our Planet, human city pioneer and international scientific advisor Carlos Moreno delivers an exciting and insightful discussion of the deceptively simple and revolutionary idea that everyday destinations like schools, stores, and offices should only be a short walk or bike ride away from home. This book tells the story of an idea that spread from city to city, describing a new way of looking at living that addresses many of the most intractable challenges of our time. Hundreds of mayors worldwide have already embraced the concept as a way to help recover from the pandemic, and the idea continues to gain speed. You'll learn why more and more cities are planning to make cars far less necessary for contemporary city-dwellers and how they're planning to achieve that goal. You'll also find: Strategies for cities to recover and adapt to benefit residents, saving them precious time Techniques to change the habits of automobile-dependent city residents and maximize social benefits of living in a human-centric city Scientifically developed, research-backed solutions for enduring urban issues and problems Deeply committed to science, progress, and creativity, Moreno presents an essential and timely resource in The 15-Minute City, which will prove invaluable to anyone with an interest in modern and innovative approaches to consistently challenging urban issues that have bedeviled policy makers and city residents since the invention of the car.

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Source

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• Type de publi. : Pré-publication, Document de travail
• Date de publi. : 07/05/2024
• 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 Lucas 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 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 ArceEloisa ArenaJean-Francois ArguinSpyros ArgyropoulosJan-Hendrik ArlingOlivier ArnaezHannah ArnoldGiacomo ArtoniHaruka AsadaKanae AsaiShoji AsaiNedaa Alexandra AsbahKetevi 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 BarelKevin Nicholas BarendsTeresa BarillariMartin BarisitsTim BarklowPetr BaronDiego BaronToni BaroncelliAlan BarrJackson BarrBarreiro Barreiro AlonsoJoao Barreiro Guimaraes da CostaUriel BarronMaura BarrosSergey BarsovFalk 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KvitaTony KwanNicholas KyriacouLauri LaatuCarlos Lacasta LlacerFrancesco LacavaHeiko Markus LackerDidier LacourNisha LadEvgueni LadyginArthur LafargeBertrand LaforgeTheodota LagouriFatima Zahra LahbabiStan LaiJoseph Earl LambertSabine Wedam LammersWalter LamplChristos LampoudisGeorgios LamprinoudisAlec LancasterEric Christian LanconUlrich LandgrafMurrough LandonValerie LangOda Kristin Berg LangrekkenAndrew James LankfordFrancesco LanniKerstin LantzschAgostino LanzaJean-Francois LaporteTommaso LariFederico Lasagni ManghiMario LassnigVera LatonovaAlexandre LaurierSean Dean LawlorZak LawrenceRoxani LazaridouMassimo LazzaroniBrian LeElise Maria Le Boulicaut EnnisLuc Tomas Le PottierBlaz LebanAlexandre LebedevMatt LeblancFabienne LedroitShih-Chang LeeSuhyun LeeTing Fung LeeLerothodi Leonard LeeuwHelena LefebvreMichel LefebvreCharles LeggettGiovanna Lehmann MiottoMatthew LeighWilliam Axel LeightWaltteri LeinonenAntonios LeisosMarco Lisboa LeiteClara Elisabeth LeitgebRupert LeitnerKatharine 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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 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

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Résumé : Several processes studied by the ATLAS experiment at the Large Hadron Collider produce low-momentum $b$-flavored hadrons in the final state. This paper describes the calibration of a dedicated tagging algorithm that identifies $b$-flavored hadrons outside of hadronic jets by reconstructing the soft secondary vertices originating from their decays. The calibration is based on a proton-proton collision dataset at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 140 fb$^{-1}$. Scale factors used to correct the algorithm's performance in simulated events are extracted for the $b$-tagging efficiency and the mistag rate of the algorithm using a data sample enriched in $t\bar{t}$ events. Several orthogonal measurement regions are defined, binned as a function of the multiplicities of soft secondary vertices and jets containing a $b$-flavored hadron in the event. The mistag rate scale factors are estimated separately for events with low and high average number of interactions per bunch crossing. The results, which are derived from events with low missing transverse momentum, are successfully validated in a phase space characterized by high missing transverse momentum and therefore are applicable to new physics searches carried out in either phase space regimes.

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Source

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• Type de publi. : Pré-publication, Document de travail
• Date de publi. : 02/05/2024
• 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 BaldiniHaoran BaoJuan Baptista de Souza LeiteMatteo BarbettiIvanildo Rui BarbosaRoger BarlowMikhail BarnyakovSergey BarsukWilliam BarterMatteo BartoliniJustin BartzFedor BaryshnikovJan-Marc BaselsGiovanni BassiBaasansuren BatsukhAlexander BattigAurelio BayAnja BeckMaik BeckerFranco BedeschiIgnacio BediagaSamuel 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 BolzonellaNikolay BondarFederica BorgatoSilvia BorghiMartino BorsatoJozef Tomasz BorsukSonia Amina BouchibaThemistocles BowcockAlexandre BoyerConcezio BozziMatthew John BradleyAlexandre Brea RodriguezNils BreerJolanta BrodzickaArnau Brossa GonzaloJames David BrownDavide BrunduEmma BuchananAnnarita 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• Organismes : 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 Leprince-Ringuet Laboratoire d'Annecy de Physique des Particules Laboratoire Leprince-Ringuet 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 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 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 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 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 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 de Clermont Laboratoire de Physique des 2 Infinis Irène Joliot-Curie

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Résumé : The decays of the $B^{+}$ meson to the final state $D^{*-}D^{+}_{s}\pi^{+}$ are studied in proton-proton collision data collected with the LHCb detector at centre-of-mass energies of 7, 8, and 13 TeV, corresponding to a total integrated luminosity of 9 fb$^{-1}$. The ratio of branching fractions of the $B^{+}\to D^{*-}D^{+}_{s}\pi^{+}$ and $B^{0}\to D^{*-}D^{+}_{s}$ decays is measured to be $0.173\pm 0.006\pm 0.010$, where the first uncertainty is statistical and the second is systematic. Using partially reconstructed $D^{*+}_{s}\to D^{+}_{s}\gamma$ and $D^{+}_{s}\pi^{0}$ decays, the ratio of branching fractions between the $B^{+}\to D^{*-}D^{*+}_{s}\pi^{+}$ and $B^{+}\to D^{*-}D^{+}_{s}\pi^{+}$ decays is determined as $1.31\pm 0.07\pm 0.14$. An amplitude analysis of the $B^{+}\to D^{*-}D^{+}_{s}\pi^{+}$ decay is performed for the first time, revealing dominant contributions from known excited charm resonances decaying to the $D^{*-}\pi^{+}$ final state. No significant evidence of exotic contributions in the $D^{+}_{s}\pi^{+}$ or $D^{*-}D^{+}_{s}$ channels is found. The fit fraction of the scalar state $T_{c\bar{s} 0}^{\ast}(2900)^{++}$ observed in the $B^{+}\to D^{-}D^{+}_{s}\pi^{+}$ decay is determined to be less than 2.3% at a 90% confidence level.

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