Philippe JEAN-PIERRE

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• Type de publi. : Pré-publication, Document de travail
• Date de publi. : 03/09/2025
• Auteurs : Nikola BesicNicolas PicardCédric VégaJean-Pierre RenaudMartin SchwartzMilena PlanellsPhilippe Ciais
• Organismes : Recherche, développement et innovation Commissariat à l'énergie atomique et aux énergies alternatives Centre National de la Recherche Scientifique Université Paris-Saclay Institut Pierre-Simon-Laplace Centre d'études spatiales de la biosphère Institut National de Recherche pour l’Agriculture, l’Alimentation et l’Environnement Centre d'études spatiales de la biosphère Centre National de la Recherche Scientifique Commissariat à l'énergie atomique et aux énergies alternatives Institut Pierre-Simon-Laplace Laboratoire des Sciences du Climat et de l'Environnement [Gif-sur-Yvette]

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Résumé : The development of high resolution mapping models of forest attributes based on employing machine or deep learning techniques has increasingly accelerated in the last couple of years. The consequence of this is the widespread availability of multiple sources of information, which can either lead to a potential confusion, or to a possibility to get an "extended” insight into the state of our forests by interpreting these sources jointly. This contribution aims at addressing the latter, by relying on the Bayesian model averaging (BMA) approach. BMA is a method that can be used in building a consensus from an ensemble of different model predictions. It can be seen as weighted mean of different predictions with weights reflecting the predictive performances of different models, or as a finite mixture model which estimates the probability that each observation from the independent validation dataset has been generated by one of the models belonging to the ensemble. BMA can thus be used to diagnose and understand the difference in the predictions and to possibly interpret them. The predictions in our case are the forest canopy height estimations for the metropolitan France coming from 5 different AI models [1-5], while the independent validation dataset comes from the French National Forest Inventory (NFI) disposing with some 6000 plots per year, distributed across the territory of interest. For every plot we have several measurements/estimations of the forest canopy height out of which the following two are considered in this study: h_m – the maximum total height (from the tree's base level to the terminal bud of the tree's main stem) measured within the plot, and h_dom – the average height of the seven largest dominant trees per hectare. In this contribution we present for every considered plot the dominant model with respect to both references i.e. the model having the highest probability to be the one generating measurements/estimations at NFI plot (h_m and h_dom). We present as well as the respective inter-model and the intra-model variance estimations, allowing us to propose a series of hypotheses concerning the established differences between predictions of individual models in function of their specificities. [1] Schwartz, M., et al.: FORMS: Forest Multiple Source height, wood volume, and biomass maps in France at 10 to 30 m resolution based on Sentinel-1, Sentinel-2, and Global Ecosystem Dynamics Investigation (GEDI) data with a deep learning approach, Earth Syst. Sci. Data, 15, 4927–4945, 2023, https://doi.org/10.5194/essd-15-4927-2023 [2] Lang, N., et al.: A high-resolution canopy height model of the Earth, Nat Ecol Evol 7, 1778–1789, 2023. https://doi.org/10.1038/s41559-023-02206-6 [3] Morin, D. et al.: Improving Heterogeneous Forest Height Maps by Integrating GEDI-Based Forest Height Information in a Multi-Sensor Mapping Process, Remote Sens., 14, 2079. 2022, https://doi.org/10.3390/rs14092079 [4] Potapov, P., et al.: Mapping global forest canopy height through integration of GEDI and Landsat data, Remote Sensing of Environment, 253, 2021, https://doi.org/10.1016/j.rse.2020.112165. [5] Liu, S. et al.: The overlooked contribution of trees outside forests to tree cover and woody biomass across Europe, Sci. Adv. 9, eadh4097, 2023, 10.1126/sciadv.adh4097.

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• Type de publi. : Pré-publication, Document de travail
• Date de publi. : 01/09/2025
• Auteurs : Roel AaijAhmed Sameh Wagih AbdelmottelebCarlos Abellan BetetaFernando Jesus AbudinénThomas AckernleyAyomide Matthew AdefisoyeBernardo AdevaMarco AdinolfiPatrik Harri AdlarsonChristina AgapopoulouChristine Angela AidalaZiad AjaltouniSimon AkarKazuyoshi AkibaPietro AlbicoccoJohannes AlbrechtRamunas AleksiejunasFederico AlessioPaula Alvarez CartelleRenaud AmalricSandra AmatoJake Lewis AmeyYasmine AmhisLiupan AnLucio AnderliniMartin AnderssonPasquale AndreolaMirco AndreottiSergio Andres EstradaAlessia AnelliDong AoCarolina ArataFlavio ArchilliZaratsyan AregMatteo ArgentonSergio Arguedas CuendisLisa ArnoneAlexander ArtamonovMarina ArtusoElie AslanidesRita Ataíde da SilvaMichele AtzeniBenjamin AudurierJuliette AuthierDavid BacherIrene Bachiller PereaSebastian BachmannMarie BachmayerJohn BackPablo Baladron RodriguezVladislav BalaguraAnna BalboniWander BaldiniZachary BaldwinLuca BalzaniHaoran BaoJuan Baptista de Souza LeiteCarlos Javier Barbero PretelMatteo BarbettiIvanildo Rui BarbosaRoger BarlowMikhail BarnyakovSergey BarsukWilliam BarterJustin BartzSaliha BashirBaasansuren BatsukhPiera BattistaAurelio BayAnja BeckMaik BeckerFranco BedeschiIgnacio BediagaNoah Albin BehlingSamuel BelinAlberto BellavistaKonstantin BelousIlia BelovIvan BelyaevGaya BenaneGiovanni BencivenniEli Ben-HaimAlexander BerezhnoyRoland BernetSergi Bernet AndresAlessandro BertolinChristopher BetancourtFederico BettiJosh BexIaroslava BezshyikoOleg BezshyykoJihyun 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 BolzonellaRiccardo BonacciNikolay BondarAleksandar BordeliusFederica BorgatoSilvia BorghiMartino BorsatoJozef Tomasz BorsukElia BottalicoSonia Amina BouchibaMarcelo BovillThemistocles BowcockAlexandre BoyerConcezio BozziJames Daniel BrandenburgAlexandre Brea RodriguezNils BreerJolanta BrodzickaArnau Brossa GonzaloJames David BrownDavide BrunduEmma BuchananMarta Burgos MarcosAodhan Tomas BurkeChristopher BurrClarissa ButiJordy Sebastiaan ButterJan BuytaertWiktor ByczynskiSandro CadedduHao CaiYuman CaiAlois CailletRoberto CalabreseSaul Calderon RamirezLukas CaleficeMarta CalviMiriam Calvo GomezPatricia Camargo MagalhaesJose Ivan Cambon BouzasPierluigi CampanaDaniel Hugo Campora PerezAngel Fernando Campoverde QuezadaSimone CapelliMarco CaporaleLorenzo CapriottiRonald Gerardo Caravaca-MoraAngelo CarboneLidia Carcedo SalgadoRoberta CardinaleAlessandro CardiniPaolo CarnitiLeon David CarusAdrian Casais VidalRowina CasparyGianluigi CasseMarco CattaneoGiovanni CavalleroViola CavalliniSara CelaniIrene CelestinoSara CesareFelipe Cesario Laterza LopesAbbie Jane ChadwickIbrahim ChahrourHao ChangMatthew CharlesPhilippe CharpentierEvridki ChatzianagnostouRacha CheaibMaximilien ChefdevilleChen ChenJou-An ChenShanzhen ChenZewen ChenMostafa CherifAleksei ChernovSerhii ChernyshenkoXenofon ChiotopoulosVeronika ChobanovaMarcin ChrzaszczAleksei ChubykinVladimir ChulikovPaolo CiambroneXabier Cid VidalGregory CiezarekPierfrancesco CifraPeter ClarkeMarco ClemencicHarry CliffJoel ClosierCarlos Eduardo Cocha ToapaxiVictor CocoJulien CoganEric CognerasLucian CojocariuSpencer Edward CollavitiPaula CollinsTommaso ColomboMarco ColonnaAlbert Comerma-MontellsLiliana CongedoJames ConnaughtonAndrea ContuNaomi CookeGiulio CordovaChristian Andres CoronelImanol CorredoiraAnthony CorreiaGloria CortiJozie Cottee MeldrumBenjamin CouturierDaniel Charles CraikMelissa Maria Cruz TorresEsteban Curras RiveraRobert CurrieCesar Luiz da SilvaShakhzod DadabaevLingyun DaiXinchen DaiElena Dall'OccoJeremy DalsenoCarmelo d'AmbrosioJessy DanielPhilippe d'ArgentGabriella DarzeAlexander DavidsonJonathan Edward DaviesOscar de Aguiar FranciscoCamilla de AngelisFederico de BenedettiJan de BoerKristof de BruynStefano 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van VeghelGerardo VasquezRicardo Vazquez GomezPablo Vazquez RegueiroCarlos Vázquez SierraStefania VecchiJavier Velilla SernaJaap VelthuisMichele VeltriAravindhan VenkateswaranMichele VerdogliaMika VesterinenWren VetensDavid Vico BenetPol Vidrier VillalbaMaria Vieites DiazXavier Vilasis-CardonaEva Vilella FiguerasAndrea VillaPascal VincentBeatriz VivacquaFelicia Carolin VolleDorothea Vom BruchNikolai VoropaevKimberley VosConstantinos VrahasJan Peter WagnerJohn WalshEliot Jane WaltonGuanyue WanAnqi WangBoxin WangChishuai WangGanrong WangHong-Jian WangJialu WangJianchun WangJianqiao WangJike WangMengzhen WangNanyang WangRui WangXiao WangXiaolin WangXiaohan WangYilong WangYuhao WangYinghao WangZhenzi WangZiyi WangJake Alexander WardMark WaterlaatNigel WatsonDavid WebsdaleYajing WeiZheng WeidaJohn WendelBenedict Donald C WesthenryCallum James WhiteMark WhiteheadEleanor WhiterAidan Richard WiederholdDirk WiednerMax WiegertjesCharlie WildGuy WilkinsonMichael K WilkinsonMike WilliamsMorag Jean WilliamsMark Richard James WilliamsRichard Morgan WilliamsSean James WilliamsZak WilliamsFergus WilsonMichael Andreas WinnWojciech WislickiMariusz WitekLukas WitolaTom WolfElla WoodGuy WormserStephen WottonHangyi WuJie WuXiangyu WuYanxi WuZhenhong WuKenneth WyllieShu XianZhiyu XiangYuehong XieTianyu XingAo XuLi XuLiangjun XuMenglin XuZehua XuZhihao XuZijun XuKang YangXueting YangYouhua YangZhenwei YangVsevolod YeroshenkoHo Yin Dereck YeungHang YinXiaoyue YinChenxu YuJiesheng YuXuhao YuanYuan YuanEttore ZaffaroniJilberto Antonio Zamora SaaMikhail ZavertyaevMilosz ZdybalFrancesco ZenesiniCheng ZengMing ZengChenjia ZhangDongliang ZhangJianyu ZhangLiming ZhangRanyu ZhangShulei ZhangShunan ZhangYanxi ZhangYuge ZhangZhicai ZhangYa ZhaoAlexey ZhelezovShuang ZhengXutao ZhengYangheng ZhengTianwen ZhouXiaokang ZhouYixiong ZhouValeriia ZhovkovskaLinxuan ZhuXianglei ZhuXiaoyu ZhuYibo ZhuValery ZhukovJiahui ZhuoQuan ZouDavide ZulianiGianluca Zunica
• Organismes : Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont Laboratoire de Physique de Clermont Laboratoire de Physique Nucléaire et de Hautes Énergies 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 Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Institut de Recherches sur les lois Fondamentales de l'Univers 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 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 de Physique Nucléaire et de Hautes Énergies 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 de Clermont Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique Nucléaire et de Hautes Énergies 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 Centre de Physique des Particules de Marseille Laboratoire Leprince-Ringuet Centre de Physique des Particules de Marseille 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 de Clermont 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 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 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 Centre de Physique des Particules de Marseille Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire Leprince-Ringuet 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 de Physique Nucléaire et de Hautes Énergies Laboratoire Leprince-Ringuet Laboratoire Leprince-Ringuet Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique de Clermont Laboratoire de Physique de Clermont Centre de Physique des Particules de Marseille Laboratoire Leprince-Ringuet Laboratoire de Physique de Clermont Institut de Recherches sur les lois Fondamentales de l'Univers 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 Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille Laboratoire Leprince-Ringuet Institut de Recherches sur les lois Fondamentales de l'Univers 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 Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies Centre de Physique des Particules de Marseille 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 Leprince-Ringuet Laboratoire de Physique des 2 Infinis Irène Joliot-Curie

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Résumé : A search for the charmless baryonic decay $B^+\to \barΛ p\bar{p}p$ is performed using proton-proton collision data recorded by the LHCb experiment, corresponding to an integrated luminosity of 5.4~$\text{fb}^{-1}$. The branching fraction for this decay is measured for the first time relative to that of the topologically similar decay $B^+\to J/ψK^+$, with $J/ψ\to \barΛ p K^-$. The branching fraction is measured to be \mbox{$\mathcal{B}(B^+\to \barΛ p\bar{p}p) = (2.08 \pm 0.34 \pm 0.12 \pm 0.26) \times 10^{-7}$}, where the first uncertainty is statistical, the second is systematic, and the third arises from the uncertainty in the normalization channel branching fraction. The $CP$ asymmetry is measured to be $\mathcal{A}_{CP}=(5.4\pm 15.6\pm 2.4)\%$, where the uncertainties are statistical and systematic. The background-subtracted invariant-mass distributions of $\barΛp$ and $\bar{p}$ pairs exhibit pronounced enhancements at both kinematic thresholds, in contrast to a uniform phase-space distribution.

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/09/2025
• Auteurs : Guanghui FuLucia NichelliDarío Herrán de la GalaSophie LoizillonCamile BousfihaRomain ValabregueAgusti AlentornKhê Hoang-XuanBertrand MathonCarole SoussainJean-Pierre MarolleauJérôme PaillassaLuc TaillandierPhilippe AgapéAnna SchmittO. ChinotGuido AhleDidier DormontCaroline HouillierStéphane LehéricyOlivier Colliot
• Organismes : Institut du Cerveau = Paris Brain Institute Institut du Cerveau = Paris Brain Institute CHU Pitié-Salpêtrière [AP-HP] Algorithms, models and methods for images and signals of the human brain = Algorithmes, modèles et méthodes pour les images et les signaux du cerveau humain [ICM Paris] Institut du Cerveau = Paris Brain Institute Sorbonne Université Equipe Neuroingénierie des systèmes pour modéliser et interfacer les réseaux cérébraux = Systems neuroengineering to model and interface brain networks [ICM Paris] Institut du Cerveau = Paris Brain Institute Instabilité des microsatellites et cancers [CRSA] CHU Pitié-Salpêtrière [AP-HP] Institut du Cerveau = Paris Brain Institute CHU Pitié-Salpêtrière [AP-HP] Institut Curie - Saint Cloud CHU Amiens-Picardie HEMATIM - Hématopoïèse et immunologie - UR UPJV 4666 Centre Hospitalier Universitaire d'Angers Service de Neuro-Oncologie [CHRU Nancy] Centre de Recherche en Automatique de Nancy Institut de Cancérologie de l'Ouest [Angers/Nantes] Institut Bergonié [Bordeaux] Institut de neurophysiopathologie Neuro-Oncologie [Hôpital de la Timone - APHM] Hôpitaux Civils de Colmar Algorithms, models and methods for images and signals of the human brain = Algorithmes, modèles et méthodes pour les images et les signaux du cerveau humain [ICM Paris] Assistance publique - Hôpitaux de Paris (AP-HP) CHU Pitié-Salpêtrière [AP-HP] Institut du Cerveau = Paris Brain Institute Institut du Cerveau = Paris Brain Institute CHU Pitié-Salpêtrière [AP-HP] Institut du Cerveau = Paris Brain Institute Algorithms, models and methods for images and signals of the human brain = Algorithmes, modèles et méthodes pour les images et les signaux du cerveau humain [ICM Paris]
• Publié dans Radiology: Imaging Cancer le 05/10/2022

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Résumé : Purpose To develop and validate a deep learning model for automatic segmentation of primary central nervous system lymphoma (PCNSL) at postcontrast T1-weighted MRI. Materials and Methods Data were retrospectively collected from patients with pathologically proven immunocompetent PCNSL between September 2010 and February 2022. Postcontrast T1-weighted MRI scans were used to train and validate a deep learning model based on the nnU-Net framework. Manual segmentation by neuroradiologists served as the reference standard. The model was trained using an internal dataset from a single center and tested on both internal and external test sets from seven additional centers. Performance was assessed using Dice score, mean average surface distance, and F1 score. Statistical comparisons were performed using Mann-Whitney U test and bootstrap resampling for CIs. Results The study included 135 patients (68 female, 66 male, and one of unspecified sex; internal dataset: mean age ±SD, 67.0 years ± 12.0; external dataset: mean age, 75.5 years ± 13.6). The model achieved a mean Dice score of 0.84 (95% CI: 0.79, 0.88) on the internal test set (n = 44) and 0.88 (95% CI: 0.84, 0.91) on the external test set (n = 48), with no evidence of a difference between test sets (P = .59). Performance varied by lesion type; accuracy was highest in homogeneous discrete lesions, and performance was slightly decreased when numerous poorly defined infracentimetric lesions occurred. Strong volumetric correlation was observed between automatic and manual segmentations (internal: r = 0.99, P < .001; external: r = 0.98, P < .001). Conclusion A deep learning model achieved accurate and robust automatic segmentation of PCNSL across multiple clinical centers with different MRI acquisition parameters.

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Fichiers liés : postprint.pdf

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Source

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• Type de publi. : Pré-publication, Document de travail
• Date de publi. : 01/09/2025
• Auteurs : Aram HayrapetyanVladimir MakarenkoArmen TumasyanWolfgang AdamJanik Walter AndrejkovicLisa BenatoThomas BergauerMarko DragicevicCristina GiordanoPriya Sajid HussainManfred JeitlerNatascha KrammerAng LiDietrich LikoMark MatthewmanIvan MikulecJochen SchieckRobert SchöfbeckDennis SchwarzMaryam ShooshtariMangesh SonawaneWolfgang WaltenbergerClaudia-Elisabeth WulzTahys JanssenHyejin KwonDaniel Ocampo HenaoThomas van LaerPierre van MechelenJas BierkensNordin BreugelmansJorgen d'HondtSoumya DansanaAlexandre de MoorMartin DelcourtFelix HeyenYanwen HongPavlo KashkoSteven LowetteInna MakarenkoDenise MüllerJuhee SongStefaan TavernierMichael TytgatGerrit Patrick van OnsemSenne van PutteDavid VanneromBugra BilinBarbara ClerbauxAloke Kumar DasIsabelle de BruynGilles de LentdeckerHugues EvardLaurent FavartParaskevas GianneiosAli KhalilzadehFakhri Alam KhanAndrea MalaraMuhammad Aamir ShahzadLaurent ThomasMax Vanden BemdenCatherine Vander VeldePascal VanlaerFengwangdong ZhangMaarten de CoenDidar DoburGul GokbulutJoscha KnolleDavid MarckxKirill SkovpenAdina Maria TomaruNiels van den BosscheJan van der LindenJules VandenbroeckLiam WezenbeekSamuel BeinAnna BeneckeAgni BethaniGiacomo BrunoAlessandra CappatiJerome de Favereau de JeneretChristophe DelaereAndrea GiammancoAhmet Oguz GuzelVincent LemaitreJindrich LidrychPaul MalekPaola MastrapasquaSemra TurkcaparGilvan AlvesMapse Barroso Ferreira FilhoEduardo CoelhoCarsten HenselThales Menezes de OliveiraClemencia Mora HerreraPatricia Rebello TelesMariana SoeiroEdmilson José Tonelli ManganoteAntonio Vilela PereiraWalter Luiz Aldá JúniorHelena Brandao MalbouissonWagner CarvalhoJose ChinellatoMatheus Costa ReisEliza Melo da CostaGustavo Gil da SilveiraDilson de Jesus DamiaoSandro Fonseca de SouzaRaphael Gomes de SouzaSilas JesusTulio Laux KuhnMatheus MacedoKevin Mota AmariloLuiz MundimHelio NogimaJoao Pedro PinheiroAlberto SantoroAndre SznajderMauricio ThielFelipe Torres da Silva de AraujoCesar Augusto BernardesFlorian DamasThiago TomeiEduardo de Moraes GregoresBruno Lopes da CostaIsabela Maietto SilverioPedro G MercadanteSergio F NovaesBreno OrzariSandra PadulaValerie ScheurerAleksandar AleksandrovGeorgy AntchevPetar DanevRoumyana HadjiiskaPlamen IaydjievMariana ShopovaGeorgi SultanovAnton DimitrovLeander LitovBorislav PavlovPeicho PetkovAnton PetrovSumit KeshriDavid Nicolas Laroze NavarreteShalini ThakurWilliam BrooksTongguang ChengTahir JavaidLong WangLi YuanZhen HuZhengchen LiangJinfeng LiuXining WangGuo-Ming ChenHe-Sheng ChenMingshui ChenYe ChenQingfeng HouXiaonan HouFabio IemmiChun-Hua JiangAnshul KapoorHongbo LiaoGeliang LiuZhenan LiuJia-Ning SongShaowei SongJunquan TaoChu WangJin WangHuaqiao ZhangJingzhou ZhaoAntonis AgapitosYong BanAlexandra Carvalho Antunes de OliveiraSen DengBotao GuoQianying GuoChuqiao JiangAndrew LevinCongqiao LiQiang LiYajun MaoSitian QianSi-Jin QianXuelong QinClaudio QuarantaXiaohu SunDayong WangJin WangHeng YangMingtao ZhangYuzhe ZhaoChen ZhouShuai YangZhengyun 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Résumé : This paper presents a search for a Higgs boson produced in association with a charm quark (cH) which allows to probe the Higgs-charm Yukawa coupling strength modifier $κ_\mathrm{c}$. Higgs boson decays to a pair of W bosons are considered, where one W boson decays to an electron and a neutrino, and the other \PW boson decays to a muon and a neutrino. The data, corresponding to an integrated luminosity of 138 fb$^{-1}$, were collected between 2016 and 2018 with the CMS detector at the LHC at a center-of-mass energy of $\sqrt{s}$ = 13 TeV. Upper limits at the 95% confidence level (CL) are set on the ratio of the measured yield to the standard model expectation for cH production. The observed (expected) upper limit is 1065 (506). When combined with the previous search for cH in the diphoton decay channel of the Higgs boson, the limits are interpreted as observed (expected) constraints at 95% CL on the value of $κ_\mathrm{c}$, $\lvertκ_\mathrm{c}\rvert$ $\lt$ 47 (51).

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