Philippe JEAN-PIERRE

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• Type de publi. : Article dans une revue
• Date de publi. : 16/10/2025
• Auteurs : Pierre BigotZine-Eddine KheneRomain BoissierLaurence AlbigesJean-Christophe BernhardOlivier ChapetJean-Michel CorreasStéphane de VergieNicolas DoumercMatthieu FerraguAlexandre IngelsGaëlle MargueYann NeuzilletIdir OuzaidCaroline PettenatiNathalie Rioux-LeclercqThibaut WaeckelPhilippe BarthélémyMorgan Rouprêt
• Organismes : Comité de cancérologie de l’Association française d’urologie Centre Hospitalier Universitaire d'Angers Centre Hospitalier Universitaire de Rennes [CHU Rennes] = Rennes University Hospital [Pontchaillou] Institut de recherche en santé, environnement et travail CHU Pitié-Salpêtrière [AP-HP]
• Publié dans French Journal of Urology le 18/12/2024

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Résumé : The 2025 update of the French guidelines for localized renal cell carcinoma highlights several major advances. Renal biopsy reaffirms its central role in guiding therapeutic decisions and reducing overtreatment, with growing evidence supporting a broader "biopsy-all" strategy. Active surveillance is now established as a safe and effective option for small renal masses, including selected complex cystic lesions, providing oncological outcomes comparable to immediate intervention. Among alternative approaches, stereotactic body radiotherapy has emerged as a credible and well-tolerated treatment for medically inoperable patients. In hereditary syndromes, progress includes improved characterization of BAP1-TPDS-associated RCC and the expanding role of belzutifan in von Hippel-Lindau disease. From an organizational standpoint, the center-volume effect is confirmed, supporting the centralization of renal cancer surgery within authorized, high-volume centers. Novel biomarkers such as KIM-1, urinary glycosaminoglycans, and circulating DNA represent promising tools for postoperative surveillance and personalized treatment planning. In the event of metastatic progression after adjuvant pembrolizumab, enrolment in a clinical trial remains the preferred strategy. For early relapse (during or within six months after adjuvant therapy), TKI monotherapy should be prioritized, whereas recurrence between six and twelve months may justify the reintroduction of immunotherapy. Beyond twelve months after pembrolizumab, standard first-line PD-1-based combinations remain the recommended approach. Finally, for localized or oligometastatic recurrences, local treatments should be considered within a multidisciplinary tumour board.

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Fichiers liés : 1-s2.0-S2950393025001548-main.pdf

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Source

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• Type de publi. : Pré-publication, Document de travail
• Date de publi. : 16/10/2025
• Auteurs : Georges AadErlend AakvaagBraden Keim AbbottSara AbdelhameedKira AbelingNils Julius AbichtHaider AbidiMohammed AboelelaAsmaa AboulhormaHalina AbramowiczYiming AbulaitiBobby Samir AcharyaAnke AckermannClaire Adam BourdariosLeszek AdamczykSagar AddepalliMatthew John AddisonJahred AdelmanAytul AdiguzelTim AdyeTony AffolderYoav AfikMerve Nazlim AgarasAnamika AggarwalCatalin AgheorghieseiFaig AhmadovSudha AhujaXiaocong AiGiulio AielliArya AikotMalak Ait TamlihatBrahim AitbenchikhMelike AkbiyikTorsten AkessonAndrei AkimovDaiya AkiyamaNilima Nilesh AkolkarSina AktasGian Luigi AlberghiJustin AlbertUna Helena AlbertiPietro AlbicoccoGuillaume Lucas AlbouySara AlderweireldtZackary Lee AlegriaMartin AleksaIgor AlexandrovCalin AlexaTheodoros AlexopoulosFabrizio AlfonsiMalte AlgrenMuhammad AlhroobBabar AliHanadi AliShahzad AliSamuel William AlibocusMalik AlievGianluca AlimontiWael AlkakhiCorentin AllaireBenedict AllbrookeJonny AllenJulia Frances AllenPhilip Patrick AllportAlberto AloisioFrancisco AlonsoCristiano AlpigianiZainab Mohammad K AlsolamiAdrian Alvarez FernandezMario Alves CardosoMariagrazia AlviggiMohamed AlyYara Do Amaral CoutinhoAlessandro AmblerChristoph AmelungMaximilian AmerlChristoph AmesThiziri AmezzaDante AmideiBaktash AminiKyle AmirieArtem AmirkhanovSusana Patricia Amor dos SantosKieran Robert AmosDimitra AmperiadouShiwen AnChristos AnastopoulosTim AndeenJohn Kenneth AndersAdam Campbell AndersonAttilio AndreazzaStylianos AngelidakisAaron AngeramiAlexey AnisenkovAlberto AnnoviClaire AntelEgor AntipovMario AntonelliFabio AnulliMasato AokiTakumi AokiMarco AparoLudovica Aperio BellaMariano ApicellaChristian AppeltAram ApyanMichaela ArampatziSergio Javier Arbiol ValChiara ArcangelettiAyana Tamu ArceJean-Francois ArguinSpyros ArgyropoulosJan-Hendrik ArlingOlivier ArnaezHannah ArnoldGiacomo ArtoniHaruka AsadaKanae AsaiSiranush AsatryanNedaa Alexandra AsbahRachel Amy Ashby PickeringAsim Mohammed AslamKetevi Adikle AssamaganRobert AstalosSten 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VerducciChristos VergisMicael Verissimo de AraujoWouter VerkerkeJos VermeulenCaterina VernieriMakayla VessellaMichel Joseph VetterliAndreas VgenopoulosNicolas Viaux MairaTrevor VickeyOana Vickey BoeriuGeorg ViehhauserLuigi ViganiMatthias ViglMauro VillaMiguel VillaplanaElena Michelle VillhauerElisabetta VilucchiMorvan VincentManuella VincterAndrea VisibileAmbre VisiveCamilla VittoriIacopo VivarelliMariana Isabel Vivas AlbornozElena VoevodinaFabian VogelJohann Christoph VoigtPetr VokacYuriy VolkotrubLuka VombergEckhard von TorneBenedikt VormwaldKonstantin VorobevMarcel VosKatharina VossMatous VozakLubos VozdeckyNenad VranjesMarija Vranjes MilosavljevicMarcel VreeswijkNgoc Khanh VuRaphael VuillermetOlivera VujinovicIlija VukoticIshan Kiritbhai VyasJulian Friedrich WackSayaka WadaCooper WagnerJohannes Michael WagnerWolfgang WagnerShayma WahdanHernan Pablo WahlbergConnor Hilton WaitsJames William WalderRodney WalkerKatie Walkingshaw PassWolfgang WalkowiakAndie WallErik Jakob WallinTanvi WamorkarKatinka Wandall-ChristensenAonan WangAlex Zeng WangChen WangChenliang WangHaichen WangJiawei WangPeng WangPeng WangRongkun WangRui WangSong-Ming WangShudong WangTao WangTianao WangWeitao WangWei WangXiaoning WangXi WangXilin WangYuhao WangYinmiao WangZirui WangZhen WangZhichen WangChaowaroj WanotayarojAndreas WarburtonAdam Leonard WarnerbringSam WaterhouseAlan WatsonHarriet WatsonMiriam WatsonElliot WattonGordon WattsBenedict WaughJames Maitland WebbChristian WeberHannsjorg WeberMichele WeberSebastian Mario WeberChuanshun WeiYingjie WeiAnthony WeidbergEdison James WeikJens WeingartenChristian WeiserCraig John WellsTorre WenausThorsten WenglerNina Stephanie WenkeNorbert WermesMartin WesselsAndrew Mark WhartonAaron Stephen WhiteAndrew WhiteMartin John WhiteDaniel WhitesonLakmin WickremasingheWerner WiedenmannMonika WielersRenske WierdaCraig WiglesworthHenric WilkensJeremy WilkinsonDaniel WilliamsHugh WilliamsSarah Louise WilliamsStephane WillocqBenjamin James WilsonDanielle Joan Wilson-EdwardsPhilipp WindischhoferFederico WinkelFrank WinklmeierBenedict Tobias WinterMatthias WittgenMarkus WobischThomas WojtkowskiZef WolffsJulian WollrathMarcin WolterHelmut WoltersMarcus Clark WongEleanor Luise WoodwardSteven WormBarbara Krystyna WosiekKrzysztof Wieslaw WozniakSebastian WozniewskiKenneth Gibb WraightChufan WuChonghao WuJian WuMinlin WuMengqing WuSau Lan WuShaoguang WuXingyu WuJerry WuYusheng WuZhibo WuZuofei WuJonas WurzingerTerry WyattBenjamin Michael WynneStefania XellaLigang XiaMingzhe XieAnni XiongDa XuHao XuLailin XuRiley XuTairan XuYue XuZhongyukun XuRui XueBruce Donald YabsleySahal YacoobYohei YamaguchiErika YamashitaHiroki YamauchiTomohiro YamazakiYuji YamazakiSiyuan YanZhen YanHaijun YangHongtao YangSiqi YangTianyi YangXiao YangXuan YangYi-Lin YangYifan YangWei-Ming YaoCaley Luce YardleyJingbo YeShuwei YeXinmeng YeYoran YehIvan YeletskikhBeomki YeoMelissa YexleyTom Philip YildirimKohei YoritaChristopher YoungCharlie YoungNathan YoungYi YuJiarong YuanMan YuanRui YuanLuzhan YueMohamed ZaazouaBartlomiej Henryk ZabinskiImane ZahirAlessandro ZaioZuzanna Katarzyna ZakTamar ZakareishviliStefano ZambitoJilberto Zamora-SaaJiaqi ZangRiccardo ZanzotteraOta ZaplatilekChristian ZeitnitzHao ZengJiancong ZengTodd ZengerOleg ZeninTibor ZenisSeth ZenzDirk ZerwasMingjie ZhaiDengfeng ZhangGengyuan ZhangJie ZhangJinlong ZhangKaili ZhangLuxin ZhangLei ZhangPeng ZhangRui ZhangSijing ZhangTingyu ZhangYulei ZhangYuwen Ebony ZhangYangfan ZhangYixiang ZhangZhirong ZhangZhuolin ZhangZhiqing Philippe ZhangHaoran ZhaoTongbin ZhaoYuzhan ZhaoZhengguo ZhaoZihan ZhaoAlexey ZhemchugovJinchao ZhengKai ZhengXiangxuan ZhengZhi ZhengDewen ZhongBing ZhouHao ZhouNing ZhouYan ZhouYong ZhouYou ZhouChengguang ZhuJunjie ZhuXuliang ZhuYifan ZhuYingchun ZhuXuai ZhuangKonstantin ZhukovNikolai ZimineJoachim ZinsserMichal ZiolkowskiLidija ZivkovicAntonio ZoccoliKnut ZochAngelos ZografosTheodore ZorbasOlga ZormpaLukasz Zwalinski
• Organismes : Centre de Physique des Particules de Marseille Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique de Clermont Institut de Recherches sur les lois Fondamentales de l'Univers 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 des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules AstroParticule et Cosmologie Centre de Physique des Particules de Marseille Laboratoire de Physique Nucléaire et de Hautes Énergies AstroParticule et Cosmologie Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire des deux Infinis de Toulouse 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 de Clermont Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules Laboratoire d'Annecy de Physique des Particules Laboratoire d'Annecy de Physique des Particules 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 Institut de Recherches sur les lois Fondamentales de l'Univers Centre de Physique des Particules de Marseille Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique de Clermont Laboratoire d'Annecy de Physique des Particules Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique Nucléaire et de Hautes Énergies 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 Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Subatomique et de Cosmologie Laboratoire de Physique de Clermont 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 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 des 2 Infinis Irène Joliot-Curie Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille 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 Laboratoire de Physique Subatomique et de Cosmologie Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique de Clermont 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 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 Nucléaire et de Hautes Énergies Laboratoire d'Annecy de Physique des Particules Laboratoire de Physique Nucléaire et de Hautes Énergies 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 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 d'Annecy de Physique des Particules AstroParticule et Cosmologie Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire d'Annecy de Physique des Particules 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 Laboratoire de Physique des 2 Infinis Irène Joliot-Curie Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique Subatomique et de Cosmologie AstroParticule et Cosmologie Laboratoire des deux Infinis de Toulouse AstroParticule et Cosmologie 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 Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique des 2 Infinis Irène Joliot-Curie 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 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 Subatomique et de Cosmologie Institut de Recherches sur les lois Fondamentales de l'Univers Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire de Physique de Clermont Centre de Physique des Particules de Marseille 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 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 Centre de Physique des Particules de Marseille 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 Laboratoire des deux Infinis de Toulouse Laboratoire des deux Infinis de Toulouse Centre de Physique des Particules de Marseille Centre de Physique des Particules de Marseille Laboratoire des deux Infinis de Toulouse Laboratoire de Physique Nucléaire et de Hautes Énergies Laboratoire des deux Infinis de Toulouse Laboratoire de Physique des 2 Infinis Irène Joliot-Curie 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 : A search for the resonant production of a heavy scalar $X$ decaying into a Higgs boson and a lighter scalar $S$, through the process $X \rightarrow S (\rightarrow b \bar{b})H ( \rightarrow γγ)$, where the two photons are consistent with the Higgs boson decay, is performed. The search is conducted using integrated luminosities of 140 fb$^{-1}$ and 58.6 fb$^{-1}$ of proton-proton collision data at centre-of-mass energies of 13 TeV and 13.6 TeV respectively, recorded with the ATLAS detector at the Large Hadron Collider. The search is performed over the mass ranges of 170 $\leq$$m_{X}$$\leq$ 1000 GeV and 15 $\leq$$m_{S}$$\leq$ 500 GeV. No significant excess over the Standard Model background prediction is observed and limits at 95% confidence level are set on the cross-section times branching ratio $σ(X \rightarrow S (\rightarrow b \bar{b})H ( \rightarrow γγ))$ at 13 TeV, ranging from 9 fb to 0.06 fb.

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• Type de publi. : Article dans une revue
• Date de publi. : 15/10/2025
• Auteurs : Léna ParcFrançois BouchyNeil James CookNolan GrievesÉtienne ArtigauAlexandrine L’heureuxRené DoyonYuri MessiasFrederique BaronS. BarrosBjörn BennekeXavier BonfilsMarta BryanBruno Canto MartinsRyan CloutierNicolas CowanDaniel Brito de FreitasJose Renan de MedeirosXavier DelfosseElisa Delgado-MenaXavier DumusqueDavid EhrenreichPedro FigueiraJ. HernándezDavid LafrenièreIzan de Castro LeãoChristophe LovisLison MaloClaudio MeloLucille MignonChristoph MordasiniFrancesco PepeRafael ReboloJason RoweN. SantosDamien SégransanAlejandro Suárez MascareñoStéphane UdryDiana ValenciaGregg WadeManuel AbreuJosé AguiarKhaled Al MoullaGuillaume AllainRomain AllartJose Manuel Almenara VillaTomy ArialHugues AugerLuc BazinetNicolas BlindDavid BohlenderIsabelle BoisseAnne BoucherVincent BourrierSébastien BovayPedro BrancoChristopher BroegDenis BrousseauAlexandre CabralCharles CadieuxAndrés CarmonaYann CarteretZalpha ChallitaDavid CharbonneauBruno ChazelasCatherine ClarkJoão CoelhoMarion CointepasK. CollinsKevin CollinsUriel ConodEduardo CristoAna Rita Costa SilvaAntoine Darveau-BernierLaurie DauplaiseJ.-B. DelisleRoseane de Lima GomesJ. FariaDasaev FontineleThierry ForveilleYolanda FrenschJonathan GagnéFrédéric GenestLudovic GenoletJoão Gomes da SilvaFélix Gracia TémichNicole GromekOlivier HernandezMelissa HobsonH. Jens HoeijmakersNorbert HubinMarziye JafariyazaniFarbod JahandarRay JayawardhanaHans-Ulrich KäuflDan KerleyJohann KolbVigneshwaran KrishnamurthyBenjamin KungPierrot LamontagnePierre LarueHenry LeathOlivia LimGaspare Lo CurtoAllan MartinsElisabeth MatthewsJaymie MatthewsJean-Sébastien MayerStanimir MetchevLina MessamahLeslie MorantaDany MounzerNicola NariLouise NielsenAres OsbornMathieu OuelletJon OtegiLuca PasquiniVera PasseggerStefan PelletierCéline PérouxCaroline Piaulet-GhorayebMykhaylo PlotnykovEmanuela PompeiAnne-Sophie Poulin-GirardJosé Luis RasillaVladimir ReshetovJonathan Saint-AntoineMirsad SarajlicIvo SavianeRobin SchnellAlex SegoviaJulia V. SeidelArmin SilberPeter SinclairMichael SordetDanuta SosnowskaAvidaan SrivastavaAtanas StefanovMárcio TeixeiraSimon ThibaultPhilippe ValléeThomas VandalValentina VaulatoJoost WardenierBachar WehbeDrew WeissermanIvan WeversFrançois WildiVincent YarivGérard Zins
• Organismes : Observatoire Astronomique de l'Université de Genève Observatoire Astronomique de l'Université de Genève Institut de Planétologie et d'Astrophysique de Grenoble Institut de Planétologie et d'Astrophysique de Grenoble Institut de Planétologie et d'Astrophysique de Grenoble Université de Montréal Institut Trottier de Recherche sur les Exoplanètes Instituto de Astrofísica e Ciências do Espaço Département de Physique [Montréal] Institut de Planétologie et d'Astrophysique de Grenoble University of California [Berkeley] Harvard-Smithsonian Center for Astrophysics Department of Physics [McGill University] Institut de Planétologie et d'Astrophysique de Grenoble Observatoire Astronomique de l'Université de Genève Observatoire Astronomique de l'Université de Genève Institut de Planétologie et d'Astrophysique de Grenoble Institut de Planétologie et d'Astrophysique de Grenoble Institut de Planétologie et d'Astrophysique de Grenoble Institut de Planétologie et d'Astrophysique de Grenoble European Southern Observatory
• Publié dans Astronomy & Astrophysics - A&A le 28/10/2020

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Résumé : Context . The Near InfraRed Planet Searcher (NIRPS) joined HARPS on the 3.6-m ESO telescope at La Silla Observatory in April 2023, dedicating part of its Guaranteed Time Observations (GTO) program to the radial velocity follow-up of TESS planet candidates to confirm and characterize transiting planets around M dwarfs. Aims . We present the “Sub-Neptunes” subprogram of the NIRPS-GTO, aimed at investigating the composition and formation of sub-Neptunes orbiting M dwarfs. We report the first results of this program with the characterization of the TOI-756 system, which consists of TOI-756 b, a transiting sub-Neptune candidate detected by TESS, as well as TOI-756 c, an additional non-transiting planet discovered by NIRPS and HARPS. Methods . We analyzed TESS and ground-based photometry, high-resolution imaging, and high-precision radial velocities (RVs) from NIRPS and HARPS to characterize the two newly discovered planets orbiting TOI-756, as well as to derive the fundamental properties of the host star. A dedicated approach was employed for the NIRPS RV extraction to mitigate telluric contamination, particularly when the star’s systemic velocity was shown to overlap with the barycentric Earth radial velocity. Results . TOI-756 is a M1V-type star with an effective temperature of T eff ~ 3657 K and a super-solar metallicity ([Fe/H]) of 0.20±0.03 dex. TOI-756 b is a 1.24-day period sub-Neptune with a radius of 2.81 ± 0.10 R ⊕ and a mass of 9.8 −1.6 +1.8 M ⊕ . TOI-756 c is a cold eccentric (e c = 0.45 ± 0.01) giant planet orbiting with a period of 149.6 days around its star with a minimum mass of 4.05 ± 0.11 M Jup . Additionally, a linear trend of 146 m s −1 yr −1 is visible in the radial velocities, hinting at a third component, possibly in the planetary or brown dwarf regime. Conclusions . We present the discovery and characterization of the transiting sub-Neptune TOI-756 b and the non-transiting eccentric cold giant TOI-756 c. This system is unique in the exoplanet landscape, standing as the first confirmed example of such a planetary architecture around an M dwarf. With a density of 2.42 ± 0.49 g cm −3 , the inner planet, TOI-756 b, is a volatile-rich sub-Neptune. Assuming a pure H/He envelope, we inferred an atmospheric mass fraction of 0.023 and a core mass fraction of 0.27, which is well constrained by stellar refractory abundances derived from NIRPS spectra. It falls within the still poorly explored radius cliff and at the lower boundary of the Neptune desert, making it a prime target for a future atmospheric characterization with JWST to improve our understanding of this population.

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Fichiers liés : aa55684-25.pdf

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• Type de publi. : Article dans une revue
• Date de publi. : 15/10/2025
• Auteurs : Romain CeinosJean-Pierre AttalPhilippe FrançoisClaire-Adeline DantagnanElisabeth DursunLebon NicolasCarole Charavet
• Organismes : Université Côte d'Azur - Faculté de Chirurgie Dentaire Hôpital Saint-Roch [Nice] Aix-Marseille Université - Faculté des sciences médicales et paramédicales Université Paris Cité Santé orale Université Paris Cité Santé orale Université Paris Cité Santé orale Université Paris Cité Santé orale De Vinci Higher Education Santé orale Université Côte d'Azur - Faculté de Chirurgie Dentaire Centre Hospitalier Universitaire de Nice Microbiologie Orale, Immunothérapie et Santé
• Publié dans Biomatériaux Cliniques Dentaires le 05/04/2019

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Résumé : Souvent considéré comme une simple formalité marquant la fin du traitement, le débaguage orthodontique est en réalité une étape à haut risque iatrogène. Réalisé parfois de manière « précipitée », il peut entraîner des dommages irréversibles sur un émail fragilisé. Un paradoxe, compte tenu de la patience imposée durant des mois, voire des années de traitement. Bien que des données existent dans la littérature, le manque d’informations, de formation ou la sous-estimation des dégâts potentiels conduisent à sacrifier, parfois involontairement, la qualité au profit de la rapidité. Cet article propose de replacer le débaguage au centre des préoccupations cliniques. Il s’intéresse aux limites des instruments actuellement disponibles, tout en ouvrant des pistes vers une instrumentation plus précise, mieux tolérée par les tissus dentaires et compatible avec les contraintes de temps de la pratique clinique quotidienne.

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• Type de publi. : Pré-publication, Document de travail
• Date de publi. : 14/10/2025
• Auteurs : Céline BougelSébastien DejeanCaroline GiulioliPhilippe Saint-PierreNicolas SavySandrine Andrieu
• Organismes : Centre d'Epidémiologie et de Recherche en santé des POPulations Institut de Mathématiques de Toulouse UMR5219 Centre d'Epidémiologie et de Recherche en santé des POPulations Institut de Mathématiques de Toulouse UMR5219 Université de Toulouse Institut de Mathématiques de Toulouse UMR5219 Université de Toulouse Centre d'Epidémiologie et de Recherche en santé des POPulations Service Epidémiologie clinique et santé publique [CHU Toulouse]

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Résumé : Background: Clinical trials are designed to prove the efficacy of an intervention by means of model-based approaches involving parametric hypothesis testing. Issues arise when no effect is observed in the study population. Indeed, an effect may be present in a subgroup and the statistical test cannot detect it. To investigate this possibility, we proposed to change the paradigm to a data-driven approach. We selected exploratory methods to provide another perspective on the data and to identify particular homogeneous subgroups of subjects within which an effect might be detected. In the setting of prevention trials, the endpoint is a trajectory of repeated measures. In the settings of prevention trials, the endpoint is a trajectory of repeated measures, which requires the use of methods that can take data autocorrelation into account. The primary aim of this work was to explore the applicability of different methods for clustering and classifying trajectories. Methods: The Multidomain Alzheimer Preventive Trial (MAPT) was a three-year randomized controlled trial with four parallel arms (NCT00672685). The primary outcome was a composite Z-score combining four cognitive tests. The data were analyzed by quadratic mixed effects model. This study was inconclusive. Exploratory analysis is therefore relevant to investigate the use of data-driven methods for trajectory classification. The methods used were unsupervised: k-means for longitudinal data, Hierarchical Cluster Analysis (HCA), graphic semiology, and supervised analysis with dichotomous classification according to responder status. Results: Using k-means for longitudinal data, three groups were obtained and one of these groups showed cognitive decline over the three years of follow-up. This method could be applied directly to the primary outcome, the composite Z-score with repeated observations over time. With the two others unsupervised methods, we were unable to process longitudinal data directly. It was therefore necessary to choose an indicator of change in trajectories and to consider the rate of change between two measurements. For the HCA method, Ward's aggregation was performed. The Euclidean distance and rates of change were applied for the graphic semiology method. Lastly, as there were no objective criteria to define responder status, we defined our responders based on clinical criteria. Discussion: In the princeps study, the prevention trial was found to be inconclusive, likely due to the heterogeneity of the population, which may have masked a treatment effect later identified in a refined subgroup of high Beta Amyloid subjects. So, we have adopted an alternative unsupervised approach to subject stratification based on their trajectories. We could then identify patterns of similar trajectories of cognitive decline and also highlight the potential problem of a large heterogeneity of the profiles, maybe due to the final endpoint considered.

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Fichiers liés : Bougel_etal_2025.pdf

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• Type de publi. : Communication dans un congrès
• Date de publi. : 13/10/2025
• Auteurs : Mary de FeudisKin On HoLaura HenryVanna PuglieseBoris YavkinMarie-Pierre AdamNicolas GuignotJean-Sébastien LauretFabien BénédicJocelyn AchardPhilippe GoldnerSerge DesgreniersJean-François Roch
• Organismes : Institut de Recherche de Chimie Paris CY Cergy Paris Université Laboratoire Lumière, Matière et Interfaces Synchrotron SOLEIL Università degli studi di Torino = University of Turin Laboratoire Lumière, Matière et Interfaces Laboratoire Lumière, Matière et Interfaces Synchrotron SOLEIL Laboratoire Lumière, Matière et Interfaces Laboratoire des Sciences des Procédés et des Matériaux Laboratoire des Sciences des Procédés et des Matériaux Institut de Recherche de Chimie Paris Laboratoire de physique des solides denses, Department of Physics, University of Ottawa Laboratoire Lumière, Matière et Interfaces

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Résumé : Diamonds and nanodiamonds (NDs) containing quantum color centers, such as nitrogen-vacancy (NV) centers, have been widely studied in recent years for their promising applications across various fields, including cryptography and telecommunications, medical sciences, and sensing. In the context of sensing, recent studies on color centers such as silicon-vacancy (SiV) and germanium-vacancy (GeV) centers have shown great potential for measuring physical quantities like magnetic fields, temperature, and strain. This is due to their intense zero-phonon line (ZPL) optical signal, about 80% of their total luminescence, which is characteristic of group-IV color centers (G4V) [1]. In our recent papers, we demonstrated that as-grown CVD NDs containing SiV and GeV centers, featuring luminescent ZPLs and excellent photostability at room temperature, can function effectively as nanosensors of high stress and pressure conditions (up to 180 GPa) [2, 3]. To advance our research, in this work we investigate the optical properties of SiV centers in as-grown NDs at cryogenic temperatures. For SiV centers, which have spin 1/2, the fine structure should become accessible through the Jahn-Teller effect, which lifts the degeneracy at cryogenic temperatures (< 20 K). However, experiments on our as-grown NDs reveal significant spectral broadening even at around 9 K, caused by lattice strain, which prevents access to the optically addressable electronic spin states of the SiV center. To overcome this limitation, we propose an original post-treatment involving high-pressure and high-temperature (HPHT) annealing using the Paris–Edinburgh press. In fact, the gradual increase of temperature and pressure allows for control over the undesired diamond-to-graphite phase transition. HPHT annealing experiments were conducted at the PSICHE beamline of Synchrotron SOLEIL [4], where X-ray diffraction and tomography analyses enabled precise monitoring of P,T parameters and made it possible for the first time to access single fine-structure transitions of the in such SiV-NDs. References [1] C. Bradac, et al., Nat. Commun. 10, 1 (2019). [2] B. Vindolet, et al., Phys. Rev. B 106, 214109 (2022). [3] M. De Feudis, et al., Adv. Mater. Interfaces 7, 1901408 (2019). [4] L. Henry et al., J. Synchrotron Rad. 29 (2022).

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• Type de publi. : Autre publication
• Date de publi. : 10/10/2025
• Auteurs : Carole CharavetLebon NicolasJean-Pierre AttalPhilippe FrançoisClaire-Adeline DantagnanElisabeth DursunRomain Ceinos
• Organismes : Université Côte d'Azur - Faculté de Chirurgie Dentaire Centre Hospitalier Universitaire de Nice Microbiologie Orale, Immunothérapie et Santé De Vinci Higher Education Santé orale Université Paris Cité Santé orale Université Paris Cité Santé orale Université Sorbonne Paris Cité Santé orale Université Paris Cité Santé orale Université Côte d'Azur - Faculté de Chirurgie Dentaire Hôpital Saint-Roch [Nice] Aix-Marseille Université - Faculté des sciences médicales et paramédicales
• Publié dans Information Dentaire le 23/10/2020

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Résumé : Enfin le grand jour ! Celui attendu avec impatience, parfois avec un brin d’appréhension : LA dépose de l’appareil orthodontique. Ce moment symbolique où le patient, prêt à chanter « Libéré, délivré », sent souffler un vent de liberté. Un parcours de soins partagé s’achève, souvent long, ponctué de réévaluations et parfois de plusieurs appareils… Mais c’est aussi une tranche de vie vécue aux côtés des patients et de leurs familles, avec des liens qui se sont tissés au fil du temps. Et pour nous, Orthodontistes, ce moment va bien au-delà du simple retrait de l’appareil : il marque le passage du traitement actif à la phase de contention. Un vaste sujet, la contention… Mais aujourd’hui, concentrons-nous sur l’étape intermédiaire : la fameuse dépose de la colle orthodontique restante !

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Fichiers liés : Le débaguage orthodontique.pdf

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• Type de publi. : Pré-publication, Document de travail
• Date de publi. : 10/10/2025
• Auteurs : Camila GoldySamantha MoulinYutaro ShimizuGuillaume CeruttiVincent BayleMagali S GrisonYvon JaillaisDavid BouchezYohann BouttéMartine PastugliaPhilippe AndreyMarie-Cécile Caillaud
• Organismes : Reproduction et développement des plantes Reproduction et développement des plantes Laboratoire de biogenèse membranaire Reproduction et développement des plantes Reproduction et développement des plantes Laboratoire de biogenèse membranaire Reproduction et développement des plantes Institut Jean-Pierre Bourgin - Sciences du végétal Laboratoire de biogenèse membranaire Institut Jean-Pierre Bourgin - Sciences du végétal Institut Jean-Pierre Bourgin - Sciences du végétal Reproduction et développement des plantes

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Résumé : In multicellular organisms, cell division shapes tissue architecture, cell identity, and function. In walled organisms like plants, division plane orientation irreversibly defines tissue topology and is tightly regulated. While divisions often follow the shortest path enclosing cell volume, certain cells deviate, dividing perpendicular to the growth axis. Tissue-scale mechanical stress has been proposed to guide such orientation, but how these cues are integrated remains unclear. Here, we re-examine the role of the actin cytoskeleton in orienting cell division in Arabidopsis root epidermis. Combining cell biology, genetics, pharmacological treatments, 3D segmentation, and modelling, we show that actin is a central molecular actor required to establish cell division orientation against the geometrical rules, highlighting its role in integrating spatial information.

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Fichiers liés : 2025.08.18.670899v1.full.pdf

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• Type de publi. : Article dans une revue
• Date de publi. : 09/10/2025
• Auteurs : Marie-Ange FleuryLouis OhlLionel TastetMickaël LeclercqFrédéric PreciosoPierre-Alexandre MatteiRomain CapouladeKathia AbdounÉlisabeth BédardMarie ArsenaultJonathan BeaudoinMathieu BernierErwan SalaunJérémy BernardMylène ShenSébastien HechtNancy CôtéArnaud DroitPhilippe Pibarot
• Organismes : Université Laval [Québec] Linköping University Division of Cardiovascular Medicine [Univ California San Diego] Université Laval [Québec] Modèles et algorithmes pour l’intelligence artificielle Modèles et algorithmes pour l’intelligence artificielle ITX-lab unité de recherche de l'institut du thorax UMR1087 UMR6291 Centre Hospitalier Universitaire de Nantes = Nantes University Hospital Université Laval [Québec] Université Laval [Québec] Université Laval [Québec] Université Laval [Québec] Université Laval [Québec] Université Laval [Québec] Université Laval [Québec] Université Laval [Québec] Université Laval [Québec] Université Laval [Québec] Université Laval [Québec] Université Laval [Québec]
• Publié dans European Heart Journal - Digital Health le 17/02/2023

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Résumé : Aims: There is a lack of studies investigating the pathophysiologic and phenotypic distinctiveness of aortic stenosis (AS). This heterogeneity has important implications for identifying optimal intervention timing and potential medical management. This study seeks to identify phenogroups of AS using unsupervised machine learning to improve risk stratification. Methods and results: A total of 349 patients with asymptomatic AS from the PROGRESSA study were included in this analysis. Echocardiographic, clinical and blood sample data were used in the unsupervised clustering process. Longitudinal echocardiographic data were used to evaluate AS progression. Five clusters of patients were revealed using 18 variables selected by an unsupervised machine learning algorithm. Amongst them, aortic valvular phenotype, mean gradient, peak jet velocity (Vpeak), and left ventricle stroke volume were selected as discriminatory variables. Following the clustering process, characteristics differed between clusters, including age, body mass index, and sex ratio (all P < 0.001). Of note, cluster 1 showed higher AS severity at baseline with significantly higher initial Vpeak (344 [314; 376] cm/s) and calcium score (1257 [806; 1837] UA) (P < 0.001). Patients from cluster 1 had a faster AS progression (progression of Vpeak = 22 [9; 39] cm/s/year), and calcium score (213 [111; 307] UA/year) (P < 0.001). Cluster 1 was also associated with a higher composite risk of mortality and aortic valve replacement when adjusted for age, sex, and baseline AS severity (P < 0.001). Conclusion: Artificial intelligence-guided phenotypic classification revealed 5 distinct groups and enhanced risk stratification of patients with AS. This approach may be useful to optimize and individualize medical and interventional management of AS.

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Fichiers liés : ztaf115.pdf

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