Diego SANCHEZ

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2023
• Auteurs : Pablo Torres-SánchezJavier PraenaIgnacio PorrasMarta Sabaté-GilarteClaudia Lederer-WoodsOliver AberleVictor AlcayneSimone AmaducciJózef AndrzejewskiLaurent AudouinVicente BécaresVictor Babiano-SuarezMichael BacakMassimo BarbagalloFrantišek BečvářGiorgio BelliaEric BerthoumieuxJon BillowesDamir BosnarAdam BrownMaurizio BussoManuel CaamañoLuis CaballeroFrancisco CalviñoMarco CalvianiDaniel Cano-OttAdria CasanovasFrancesco CeruttiYonghao ChenEnrico ChiaveriNicola ColonnaGuillem CortésMiguel Cortés-GiraldoLuigi CosentinoSergio CristalloLucia-Anna DamoneMaria DiakakiMirco DietzCésar Domingo-PardoRugard DresslerEmmeric DupontIgnacio DuránZinovia ElemeBeatriz Fernández-DomínguezAlfredo FerrariFrancisco Javier FerrerPaolo FinocchiaroValter FurmanKathrin GöbelRuchi GargAleksandra Gawlik-RamięgaBenoit GeslotSimone GilardoniTudor GlodariuIsabel GonçalvesEnrique González-RomeroCarlos GuerreroFrank GunsingHideo HaradaStephan HeinitzJan HeyseDavid JenkinsErwin JerichaFranz KäppelerYacine KadiAtsushi KimuraNiko KivelMichael KokkorisYury KopatchMilan KrtičkaDeniz KurtulgilIon LadarescuHelmut LeebJorge Lerendegui-MarcoSergio Lo MeoSarah-Jane LonsdaleDaniela MacinaAlice MannaTrinitario MartínezAlessandro MasiCristian MassimiPierfrancesco MastinuMario MastromarcoFrancesca MatteucciEmilio-Andrea MaugeriAnnamaria MazzoneEmilio MendozaAlberto MengoniVeatriki MichalopoulouPaolo Maria MilazzoFederica MingroneAgatino MusumarraAlexandru NegretRalf NolteFrancisco OgállarAndreea OpreaNikolas PatronisAndreas PavlikJarosław PerkowskiLuciano PersantiJosé-Manuel QuesadaDésirée RadeckDiego Ramos-DovalThomas RauscherRené ReifarthDimitri RochmanCarlo RubbiaAlok SaxenaPeter SchillebeeckxDorothea SchumannGavin SmithNikolay SosninAthanasios StamatopoulosGiuseppe TaglienteJosé TainZeynep TalipAriel Tarifeño-SaldiviaLaurent Tassan-GotAndrea TsinganisJiri UlrichSebastian UrlassStanislav ValentaGianni VanniniVincenzo VarialePedro VazAlberto VenturaVasilis VlachoudisRosa VlastouAnton WallnerPhilip John WoodsTobias WrightPetar Žugec
• Organismes : Institut de Physique Nucléaire d'Orsay Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Physique Nucléaire d'Orsay Institut de Recherches sur les lois Fondamentales de l'Univers CEA Cadarache Institut de Recherches sur les lois Fondamentales de l'Univers Institut de Physique Nucléaire d'Orsay Institut de Physique Nucléaire d'Orsay
• Publié dans Physical Review C le 02/11/2020

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Résumé : Background: The ${}^{14}\mathrm{N}(n,p){}^{14}\mathrm{C}$ reaction is of interest in neutron capture therapy, where nitrogen-related dose is the main component due to low-energy neutrons, and in astrophysics, where ${}^{14}\mathrm{N}$ acts as a neutron poison in the $s$ process. Several discrepancies remain between the existing data obtained in partial energy ranges: thermal energy, keV region, and resonance region.Purpose: We aim to measure the ${}^{14}\mathrm{N}(n,p){}^{14}\mathrm{C}$ cross section from thermal to the resonance region in a single measurement for the first time, including characterization of the first resonances, and provide calculations of Maxwellian averaged cross sections (MACS). Method: We apply the time-of-flight technique at Experimental Area 2 (EAR-2) of the neutron time-of-flight (n_TOF) facility at CERN. ${}^{10}\mathrm{B}(\mathrm{n},\alpha ){}^7\mathrm{Li}$ and ${}^{235}\mathrm{U}(n,f)$ reactions are used as references. Two detection systems are run simultaneously, one on beam and another off beam. Resonances are described with the $R$-matrix code sammy.Results: The cross section was measured from subthermal energy to 800 keV, resolving the first two resonances (at 492.7 and 644 keV). A thermal cross section was obtained ($1.809\pm 0.045$ b) that is lower than the two most recent measurements by slightly more than one standard deviation, but in line with the ENDF/B-VIII.0 and JEFF-3.3 evaluations. A 1/$v$ energy dependence of the cross section was confirmed up to tens of keV neutron energy. The low energy tail of the first resonance at 492.7 keV is lower than suggested by evaluated values, while the overall resonance strength agrees with evaluations. Conclusions: Our measurement has allowed determination of the ${}^{14}\mathrm{N}(n,p)$ cross section over a wide energy range for the first time. We have obtained cross sections with high accuracy (2.5%) from subthermal energy to 800 keV and used these data to calculate the MACS for $kT=5$ to $kT=100$ keV.

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2023
• Auteurs : Shreyasi AcharyaDagmar AdamovaGianluca Aglieri RinellaMichelangelo AgnelloNeelima AgrawalZubayer AhammedShakeel AhmadSang Un AhnIshaan AhujaAlexander AkindinovMohammad Al-TuranyDmitry AleksandrovBruno AlessandroHaidar Masud AlfandaJose Ruben Alfaro MolinaBushra AliAndrea AliciNegin AlizadehvandchaliAnton AlkinJohan AlmeGiacomo AloccoTorsten AltAnna Rita AltamuraIgor AltsybeevMustafa AnaamCristian AndreiNicodemos AndreouAnton AndronicVenelin AnguelovFederico AntinoriPietro AntonioliNicole ApadulaLaurent AphecetcheHarald AppelshaeuserCarolina ArataSilvia ArcelliMauro ArestiRoberta ArnaldiJhoao Gabriel Martins Campos Almeida ArneiroIonut Cristian ArseneMesut ArslandokAndre AugustinusRalf Peter AverbeckMohd Danish AzmiHitoshi BabaAngela BadalaJoonsuk BaeYongwook BaekXiaozhi BaiRaphaelle Marie BailhacheYoshini BailungAlessandro BalbinoAlberto BaldisseriBartosz BalisDebjani BanerjeeZarina BanooRoberto BarberaFrancesco BarileLuca BarioglioMaria BarlouBanajit BarmanGergely Gabor BarnafoldiLee Stuart BarnbyValerie 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 BelokurovaGyula BencediStefania Maria BeoleYaroslav BerdnikovAnastasia BerdnikovaLuisa BergmannMihaela Gabriela BesoiuLatchezar BetevPartha Pratim BhaduriAnju BhasinMohammad Asif BhatBuddhadeb BhattacharjeeLivio BianchiNicola BianchiJaroslav BielcikJana BielcikovaJacek Bogumil BiernatAlexandre Patrick BigotAnte BilandzicGabor BiroSaikat BiswasNicolas BizéJustin Thomas BlairDmitry BlauMihail Bogdan BlidaruNora BluhmeChristoph BlumeGianluigi BocaFriederike BockTea BodovaAlexey BogdanovStefano BoiJeongsu BokLaszlo BoldizsarMarek BombaraPeter Matthew BondGermano BonomiHerve BorelAlexander BorissovAndres Gerardo Borquez CarcamoHannah BossiElena BottaYoussef El Mard BouzianiLars BratrudPeter Braun-MunzingerMarco BregantMichal BrozGiuseppe Eugenio BrunoMatthew Daniel BucklandDmitry BudnikovHenner BueschingStefania BufalinoPaul Alois BuhlerNazar BurmasovEdith Zinhle ButheleziAleksandr BylinkinSebastian Adam BysiakMengke CaiHelen Louise CainesAlberto CalivaErnesto Calvo VillarJuan Manuel Mejia CamachoPaolo CameriniFabio de Moraes CanedoMihai CarabasAitor Amatriain CarballoFrancesca CarnesecchiRobin Albert Andre CaronLeopoldo Abranches de CarvalhoJavier Ernesto Castillo CastellanosFabio CatalanoCesar Ceballos SanchezIrakli ChakaberiaPritam ChakrabortySinjini ChandraSylvain ChapelandMarielle ChartierSubhasis ChattopadhyaySukalyan ChattopadhyayTonatiuh Garcia ChavezTiantian ChengCvetan Valeriev CheshkovBrigitte CheynisVasco Miguel Chibante BarrosoDavid Dobrigkeit ChinellatoEmma Sophia ChizzaliJaeyoon ChoSoyeon ChoPeter ChochulaDhrubajyoti ChoudhuryPanagiotis ChristakoglouChristian Holm ChristensenPeter ChristiansenTatsuya ChujoMario CiaccoCorrado CicaloFederico CindoloMichael Rudolf CiupekGiulia ClaiFabio Filippo ColamariaJonathan Samuel ColburnDomenico ColellaManuel ColocciMatteo ConcasG. 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• Publié dans Phys.Rev.D le 12/11/2025

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Résumé : The production cross sections of ${\rm D^0}$ and $\Lambda^+_{\rm c}$ hadrons originating from beauty-hadron decays (i.e. non-prompt) were measured for the first time at midrapidity ($|y|<0.5$) by the ALICE Collaboration in proton-proton collisions at a center-of-mass energy $\sqrt{s}=13$ TeV. They are described within uncertainties by perturbative QCD calculations employing the fragmentation fractions of beauty quarks to baryons measured at forward rapidity by the LHCb Collaboration. The ${\rm b\overline{b}}$ production cross section per unit of rapidity at midrapidity, estimated from these measurements, is ${\rm d}\sigma_{\rm b\overline{b}}/{\rm d}y|_{|y|<0.5} = 83.1 \pm 3.5 (\mathrm{stat.}) \pm 5.4(\mathrm{syst.}) ^{+12.3}_{-3.2} (\mathrm{extrap.})\,\mu$b. The baryon-to-meson ratios are computed to investigate the hadronization mechanism of beauty quarks. The non-prompt $\Lambda^+_{\rm c}/{\rm D^0}$ production ratio has a similar trend to the one measured for the promptly produced charmed particles and to the p$/\pi^+$ and $\Lambda/{\rm K^0_S}$ ratios, suggesting a similar baryon-formation mechanism among light, strange, charm, and beauty hadrons. The $p_{\rm T}$-integrated non-prompt $\Lambda_{\rm c}/{\rm D^0}$ ratio is found to be significantly higher than the one measured in e$^+$e$^-$ collisions.

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2023
• Auteurs : Shreyasi AcharyaDagmar AdamovaGianluca Aglieri RinellaMichelangelo AgnelloNeelima AgrawalZubayer AhammedShakeel AhmadSang Un AhnIshaan AhujaAlexander AkindinovMohammad Al-TuranyDmitry AleksandrovBruno AlessandroHaidar Masud AlfandaJose Ruben Alfaro MolinaBushra AliAndrea AliciNegin AlizadehvandchaliAnton AlkinJohan AlmeGiacomo AloccoTorsten AltAnna Rita AltamuraIgor AltsybeevMustafa AnaamCristian AndreiNicodemos AndreouAnton AndronicVenelin AnguelovFederico AntinoriPietro AntonioliNicole ApadulaLaurent AphecetcheHarald AppelshaeuserCarolina ArataSilvia ArcelliMauro ArestiRoberta ArnaldiJhoao Gabriel Martins Campos Almeida ArneiroIonut Cristian ArseneMesut ArslandokAndre AugustinusRalf Peter AverbeckMohd Danish AzmiHitoshi BabaAngela BadalaJoonsuk BaeYongwook BaekXiaozhi BaiRaphaelle Marie BailhacheYoshini BailungAlessandro BalbinoAlberto BaldisseriBartosz BalisDebjani BanerjeeZarina BanooRoberto BarberaFrancesco BarileLuca BarioglioMaria BarlouBanajit BarmanGergely Gabor BarnafoldiLee Stuart BarnbyValerie 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 BelokurovaYael Antonio Vasquez BeltranGyula BencediStefania Maria BeoleYaroslav BerdnikovAnastasia BerdnikovaLuisa BergmannMihaela Gabriela BesoiuLatchezar BetevPartha Pratim BhaduriAnju BhasinMohammad Asif BhatBuddhadeb BhattacharjeeLivio BianchiNicola BianchiJaroslav BielcikJana BielcikovaJacek Bogumil BiernatAlexandre Patrick BigotAnte BilandzicGabor BiroSaikat BiswasNicolas BizéJustin Thomas BlairDmitry BlauMihail Bogdan BlidaruNora BluhmeChristoph BlumeGianluigi BocaFriederike BockTea BodovaAlexey BogdanovStefano BoiJeongsu BokLaszlo BoldizsarMarek BombaraPeter Matthew BondGermano BonomiHerve BorelAlexander BorissovAndres Gerardo Borquez CarcamoHannah BossiElena BottaYoussef El Mard BouzianiLars BratrudPeter Braun-MunzingerMarco BregantMichal BrozGiuseppe Eugenio BrunoMatthew Daniel BucklandDmitry BudnikovHenner BueschingStefania BufalinoPaul Alois BuhlerNazar BurmasovEdith Zinhle ButheleziAleksandr BylinkinSebastian Adam BysiakMengke CaiHelen Louise CainesAlberto CalivaErnesto Calvo VillarJuan Manuel Mejia CamachoPaolo CameriniFabio de Moraes CanedoMihai CarabasAitor Amatriain CarballoFrancesca CarnesecchiRobin Albert Andre CaronLeopoldo Abranches de CarvalhoJavier Ernesto Castillo CastellanosFabio CatalanoCesar Ceballos SanchezIrakli ChakaberiaPritam ChakrabortySinjini ChandraSylvain ChapelandMarielle ChartierSubhasis ChattopadhyaySukalyan ChattopadhyayTonatiuh Garcia ChavezTiantian ChengCvetan Valeriev CheshkovBrigitte CheynisVasco Miguel Chibante BarrosoDavid Dobrigkeit ChinellatoEmma Sophia ChizzaliJaeyoon ChoSoyeon ChoPeter ChochulaDhrubajyoti ChoudhuryPanagiotis ChristakoglouChristian Holm ChristensenPeter ChristiansenTatsuya ChujoMario CiaccoCorrado CicaloFederico CindoloMichael Rudolf CiupekGiulia ClaiFabio Filippo ColamariaJonathan Samuel ColburnDomenico ColellaManuel ColocciMatteo ConcasG. 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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 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 Institut de Physique des 2 Infinis de Lyon Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Institut de Recherches sur les lois Fondamentales de l'Univers 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 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 de Clermont 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 subatomique et des technologies associées Laboratoire de Physique de Clermont Institut de Recherches sur les lois Fondamentales de l'Univers Institut Pluridisciplinaire Hubert Curien Laboratoire de Physique Subatomique et de Cosmologie 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 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
• Publié dans JHEP le 31/10/2025

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Résumé : The Chiral Magnetic Wave (CMW) phenomenon is essential to provide insights into the strong interaction in QCD, the properties of the quark-gluon plasma, and the topological characteristics of the early universe, offering a deeper understanding of fundamental physics in high-energy collisions. Measurements of the charge-dependent anisotropic flow coefficients are studied in Pb-Pb collisions at center-of-mass energy per nucleon-nucleon collision $\sqrt{s_{\mathrm{NN}}}=$ 5.02 TeV to probe the CMW. In particular, the slope of the normalized difference in elliptic ($v_{2}$) and triangular ($v_{3}$) flow coefficients of positively and negatively charged particles as a function of their event-wise normalized number difference, is reported for inclusive and identified particles. The slope $r_{3}^{\rm Norm}$ is found to be larger than zero and to have a magnitude similar to $r_{2}^{\rm Norm}$, thus pointing to a large background contribution for these measurements. Furthermore, $r_{2}^{\rm Norm}$ can be described by a blast wave model calculation that incorporates local charge conservation. In addition, using the event shape engineering technique yields a fraction of CMW ($f_{\rm CMW}$) contribution to this measurement which is compatible with zero. This measurement provides the very first upper limit for $f_{\rm CMW}$, and in the 10-60% centrality interval it is found to be 26% (38%) at 95% (99.7%) confidence level.

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2023
• Auteurs : Roel AaijAhmed Sameh Wagih AbdelmottelebCarlos Abellan BetetaFernando Jesus AbudinénThomas AckernleyBernardo AdevaMarco AdinolfiHossein AfsharniaChristina AgapopoulouChristine Angela AidalaSalvatore AiolaZiad AjaltouniSimon AkarKazuyoshi AkibaJohannes AlbrechtFederico AlessioMichael AlexanderAlejandro Alfonso AlberoZakariya AliouchePaula Alvarez CartelleSandra AmatoJake Lewis AmeyYasmine AmhisLiupan AnLucio AnderliniMartin AnderssonAleksei AndreianovMirco AndreottiDimitra AndreouDong AoFlavio ArchilliAlexander ArtamonovMarina ArtusoElie AslanidesMichele AtzeniBenjamin AudurierSebastian BachmannMarie BachmayerJohn BackAurelien Bailly-ReyrePablo Baladron RodriguezVladislav BalaguraWander BaldiniJuan Baptista de Souza LeiteMatteo BarbettiRoger BarlowSergey BarsukWilliam BarterMatteo BartoliniFedor BaryshnikovJan-Marc BaselsGiovanni BassiBaasansuren BatsukhAlexander BattigAurelio BayAnja BeckMaik 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 BiekerNicolo Vladi BiesuzSimone BifaniPierre BilloirAlice BiolchiniMatthew BirchFionn Caitlin Ros BishopAlexander BitadzeAndrea BizzetiMichele Piero BlagoThomas BlakeFrederic BlancSteven BluskDana BobulskaJulian Alexander BoelhauveOscar Boente GarciaThomas BoettcherAlexey BoldyrevNikolay BondarSilvia BorghiMartino BorsatoJozef Tomasz BorsukSonia Amina BouchibaThemistocles BowcockAlexandre BoyerConcezio BozziMatthew John BradleySvende BraunAlexandre Brea RodriguezJolanta BrodzickaArnau Brossa GonzaloDavide BrunduAnnarita BuonauraLaura BuonincontriAodhan Tomas BurkeChristopher BurrAlbert BurscheAnatoly ButkevichJordy Sebastiaan ButterJan BuytaertWiktor ByczynskiSandro CadedduHao CaiRoberto CalabreseLukas CaleficeStefano CaliRyan CalladineMarta CalviMiriam Calvo GomezPatricia Camargo MagalhaesPierluigi CampanaDaniel Hugo Campora PerezAngel Fernando Campoverde QuezadaSimone CapelliLorenzo CapriottiAngelo CarboneGiovanni CarboniRoberta CardinaleAlessandro CardiniIna CarliPaolo CarnitiLeon David CarusAdrian Casais VidalRowina CasparyGianluigi CasseMarco CattaneoGiovanni CavalleroViola CavalliniSara CelaniJacopo CerasoliDaniel CervenkovAbbie Jane ChadwickMatthew George ChapmanMatthew CharlesPhilippe CharpentierCarlos Alberto Chavez BarajasMaximilien ChefdevilleChen ChenShanzhen ChenAleksei ChernovSerhii ChernyshenkoVeronika ChobanovaSerhii CholakMarcin ChrzaszczAleksei ChubykinVladimir ChulikovPaolo CiambroneMaria Flavia CicalaXabier Cid VidalGregory CiezarekGiuseppe CiulloPeter ClarkeMarco ClemencicHarry CliffJoel ClosierJohn Leslie CobbledickVictor CocoJoao A.B CoelhoJulien CoganEric CognerasLucian CojocariuPaula CollinsTommaso ColomboLiliana CongedoAndrea ContuNaomi 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RodriguezAlexandra Paige RollingsPhilipp RoloffVladimir RomanovskiyMarcos Romero LamasAntonio Romero VidalJordan Daniel RothMarcello RotondoMatthew Scott RudolphThomas RufRamon Angel Ruiz FernandezJoan Ruiz VidalArtem RyzhikovJakub RyzkaJuan Jose Saborido SilvaNaylya SagidovaNiladribihari SahooBiagio SaittaMatteo SalomoniCristina Sanchez GrasIzaac SanderswoodRoberta SantacesariaCibran Santamarina RiosMarco SantimariaEmanuele SantovettiDanila SaraninGediminas SarpisMindaugas SarpisAlessio SartiCelestina SatrianoAlessia SattaMiroslav SaurDarya SavrinaHalime SazakLuke George Scantlebury SmeadAlessandro ScarabottoStefan SchaelSigrid ScherlManuel SchillerHeinrich SchindlerMichael SchmellingBurkhard SchmidtSebastian SchmittOlivier SchneiderAndreas SchopperMaxime SchubigerSebastian SchulteMarie Helene SchuneRainer SchwemmerBarbara SciasciaAugusto SciuccatiSara SellamAlexander SemennikovMara Senghi SoaresAntonino SergiNicola SerraLorenzo SestiniAlex SeutheYiduo ShangDesmond Mzamo 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TeubertEric ThomasDaniel James David ThompsonKayleigh Anne ThomsonHanae TilquinVincent TisserandStephane t'JampensMark TobinLuca TomassettiGiorgia TonaniXingyu TongDiego Torres Machadoda Yu TouEkaterina TrifonovaStoyan Miroslavov TrilovCarina TripplGiulia TuciAlison TullyNiels TuningArtur UklejaDaniel Joachim UnverzagtEduard UrsovAndrii UsachovAndrey UstyuzhaninUlrich UwerAlexander VagnerVincenzo VagnoniAndrea ValassiGiovanni ValentiNuria Valls CanudasMartinus van BeuzekomMaarten van DijkHubert van HeckeEric van HerwijnenMaarten van VeghelRicardo Vazquez GomezPablo Vazquez RegueiroCarlos Vázquez SierraStefania VecchiJaap VelthuisMichele VeltriAravindhan VenkateswaranMichele VeronesiMika VesterinenDaniel VieiraMaria Vieites DiazXavier Vilasis-CardonaEva Vilella FiguerasAndrea VillaPascal VincentFelicia Carolin VolleDorothea Vom BruchAlexey VorobyevVitaly VorobyevNikolai VoropaevKimberley VosRoland WaldiJohn WalshChishuai WangJialu WangJianchun WangJianqiao WangJike WangMengzhen WangRui 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• Organismes : Laboratoire de Physique de Clermont Laboratoire de Physique Nucléaire et de Hautes Énergies 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 de Physique Nucléaire et de Hautes Énergies 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 Centre de Physique des Particules de Marseille Laboratoire de Physique 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Énergies 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 de Physique de Clermont 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 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 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 de Clermont Laboratoire de Physique des 2 Infinis Irène Joliot-Curie
• Publié dans Physical Review Letters le 02/11/2020

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Résumé : The production of prompt $D^0$ mesons in proton-lead collisions in the forward and backward configurations at a center-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}} = 8.16~\mathrm{TeV}$ is measured by the LHCb experiment. The nuclear modification factor of prompt $D^0$ mesons is determined as a function of the transverse momentum $p_\mathrm{T}$, and rapidity in the nucleon-nucleon center-of-mass frame $y^*$. In the forward rapidity region, significantly suppressed production with respect to $pp$ collisions is measured, which provides significant constraints of nuclear parton distributions and hadron production down to the very low Bjorken-$x$ region of $\sim 10^{-5}$. In the backward rapidity region, a suppression with a significance of 2.0 - 3.8 standard deviations compared to nPDF expectations is found in the kinematic region of $p_\mathrm{T}>6~\mathrm{GeV}/c$ and $-3.25 Source