Philippe JEAN-PIERRE

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2021
• Auteurs : Samantha DonovanAriel AtkinsonNatalia FischerAmelia TaylorJohann KiefferJean-Philippe CrouéPaul WesterhoffPierre Herckes
• Organismes : Arizona State University [Tempe] School of Sustainable Engineering and the Built Environment School of Sustainable Engineering and the Built Environment SNF Polychemie SNF S.A. Eaux, Géochimie organique, Santé [E1 – IC2MP équipe 1] School of Sustainable Engineering and the Built Environment Arizona State University [Tempe]
• Publié dans Environmental Science : Water Research and Technology le 25/10/2020

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Résumé : Polydiallyldimethyl ammonium chloride (polyDADMAC) is the most commonly used polymer at drinking water treatment plants and has the potential to form nitrosamines, like N-nitrosodimethylamine (NDMA), if free polymer is present during the disinfection process. The composition of polyDADMAC solutions used at the industrial scale is not well understood and is difficult to analyze. This study used 1H and 13C nuclear magnetic resonance (NMR) to analyze the polymer solution composition. Both 1H and 13C NMR are powerful tools that allow study of trace impurities in the solution, structural information such as chain length, and reaction mechanisms. The information garnered through 1H and 13C NMR can be used to mitigate NDMA formation at drinking water treatment plants.

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2021
• Auteurs : Judith MichelsCatherine GenestieAriane DunantOlivier Md Msc CaronÉmilie LanoyEmeline ColombaFanny PommeretAnnie ReySébastien GouyPierre DuvillardGwénaël Le TeuffChristine LarueAude Marie SavoyeCatherine LhomméAlexandra F. LearyPhilippe MoricePatricia Pautier
• Organismes : Département de médecine oncologique [Gustave Roussy] Département de biologie et pathologie médicales [Gustave Roussy] Centre de recherche en épidémiologie et santé des populations Onco-génétique [Gustave Roussy] Centre de recherche en épidémiologie et santé des populations Centre de recherche en épidémiologie et santé des populations Département de médecine oncologique [Gustave Roussy] Département de médecine oncologique [Gustave Roussy] Centre de recherche en épidémiologie et santé des populations Pôle chirurgical et interventionnel [Gustave Roussy] Radiothérapie Moléculaire et Innovation Thérapeutique Département de biologie et pathologie médicales [Gustave Roussy] Centre de recherche en épidémiologie et santé des populations Centre de recherche en épidémiologie et santé des populations Centre de recherche en épidémiologie et santé des populations Institut Jean Godinot [Reims] Département de médecine oncologique [Gustave Roussy] Département de médecine oncologique [Gustave Roussy] Pôle chirurgical et interventionnel [Gustave Roussy] Département de médecine oncologique [Gustave Roussy]
• Publié dans Gynecologic Oncology le 25/10/2020

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Résumé : Objective: In young women, EOC is a rare disease with an uncertain genetic and biological substrate. Methods: We report a long follow-up of EOC patients treated at Gustave Roussy between 1990 and 2009. We matched young patients aged ≤30 years to randomly selected older patients aged ≥40 years according to known prognostic factors (i.e. FIGO stage, histology and surgical residual disease) and the date of diagnosis with a threshold at the year 2000 to balance the treatment procedures. Results: EOC was diagnosed in 68 patients aged ≤30 years matched with 111 patients aged ≥40 years. Low-grade (LG) (i.e. serous and endometrioid) (52%, n = 35) and mucinous (i.e. 23%, n = 16 infiltrative and 12% n = 8 expansile) tumors are prevalent. High-grade (HG) tumors are rare (7%, n = 5). Early stage diseases (53%, n = 36 FIGO I/II) are predominant. Response to platinum based chemotherapy is observed to be inferior in young patients as compared to matched older patients (ORR, 29 vs 84% p = 0.0002). For HG tumors the PFS is of 0% at 5 and 10 years in younger as compared to 30% in older patients. No difference in PFS (median 4.9 vs 9.8 ms, p = 0.58) and OS (not reached vs 15.3 ms, p = 0.47) is found overall among younger and older patients respectively. The median follow-up was 72 months (range, 11–288 months). No genetic abnormalities were found. Conclusions: Young EOC patients are most often diagnosed at an early FIGO stage with LG serous or mucinous histology. Tumors are significantly more resistant to platinum-based chemotherapy in younger patients.

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2021
• Auteurs : Albert M SirunyanArmen TumasyanWolfgang AdamFederico AmbrogiThomas BergauerMarko DragicevicJanos EröAlberto Escalante del ValleRudolf FruehwirthManfred JeitlerNatascha KrammerLukas LechnerDietrich LikoThomas MadlenerIvan MikulecFlorian Michael PittersNavid RadJochen SchieckRobert SchöfbeckMarkus SpanringSebastian TemplWolfgang WaltenbergerClaudia-Elisabeth WulzMateusz ZaruckiVladimir ChekhovskyAliaksandr LitominVladimir MakarenkoJuan Suarez GonzalezMohamed Rashad DarwishEddi A de WolfDavide Di CroceXavier JanssenTomas KelloAleksandra LelekMaxim PietersHaifa Rejeb SfarHans van HaevermaetPierre van MechelenSenne van PutteNick van RemortelFreya BlekmanEmil Sørensen BolsSimranjit Singh ChhibraJorgen d'HondtJarne de ClercqDenys LontkovskyiSteven LowetteIvan MarchesiniSeth MoortgatAlexander MortonQuentin PythonStefaan TavernierWalter van DoninckPetra van MuldersDiego BeghinBugra BilinBarbara ClerbauxGilles de LentdeckerHugo DelannoyBrian DorneyLaurent FavartAnastasia GrebenyukAmandeep Kaur KalsiInna MakarenkoLouis MoureauxLaurent PétréAndrey PopovNicolas PostiauElizabeth StarlingLaurent ThomasCatherine Vander VeldePascal VanlaerDavid VanneromLiam WezenbeekTom CornelisDidar DoburMarek GruchalaIllia KhvastunovMarek NiedzielaChristos RoskasKirill SkovpenMichael TytgatWillem VerbekeBasile VermassenMartina VitGiacomo BrunoFlorian Joel J BuryClaudio CaputoPieter DavidChristophe DelaereMartin DelcourtIzzeddin Suat DonertasAndrea GiammancoVincent LemaitreKuntal MondalJessica PrisciandaroAngela TaliercioMaksym TeklishynPietro VischiaSophie WuyckensJoze ZobecGilvan AlvesGilson Correia SilvaCarsten HenselArthur MoraesWalter Luiz Aldá JúniorEwerton Belchior Batista das ChagasHelena Brandao MalbouissonWagner CarvalhoJose ChinellatoEduardo CoelhoEliza Melo da CostaGustavo Gil da SilveiraDilson de Jesus DamiaoSandro Fonseca de SouzaJordan MartinsDiego Matos FigueiredoMiguel Medina JaimeMiqueias Melo de AlmeidaClemencia Mora HerreraLuiz MundimHelio NogimaPatricia Rebello TelesLuis Sanchez RosasAlberto SantoroSheila Mara Silva Do AmaralAndre SznajderMauricio ThielEdmilson José Tonelli ManganoteFelipe Torres da Silva de AraujoAntonio Vilela PereiraCesar Augusto BernardesLuigi CalligarisThiago TomeiEduardo de Moraes GregoresDener de Souza LemosPedro G MercadanteSergio F NovaesSandra PadulaAleksandar AleksandrovGeorgy AntchevIvan AtanasovRoumyana HadjiiskaPlamen IaydjievMilena MishevaMircho RodozovMariana ShopovaGeorgi SultanovMiroslav BonchevAnton DimitrovTodor IvanovLeander LitovBorislav PavlovPeicho PetkovAnton PetrovWenxing FangQianying GuoHanwen WangLi YuanMuhammad AhmadZhen HuYi WangEmilien ChaponGuo-Ming ChenHe-Sheng ChenMingshui ChenDuncan LeggatHongbo LiaoZhenan LiuRamkrishna SharmaAniello SpieziaJunquan TaoJoshuha Thomas-WilskerJin WangHuaqiao ZhangSijing ZhangJingzhou ZhaoAntonis AgapitosYong BanCheng ChenAndrew LevinQiang LiMeng LuXudong LyuYajun MaoSi-Jin QianDayong WangQun WangJie XiaoZhengyun YouXuyang GaoMeng XiaoCarlos AvilaAndrés CabreraCarlos FlorezJorge FragaAmal SarkarManuel Alejandro Segura DelgadoJohny JaramilloJhovanny Mejia GuisaoFelipe RamirezJosé David Ruiz AlvarezCamilo Andrés Salazar GonzálezNelson Vanegas ArbelaezDuje GiljanovicNikola GodinovicDamir LelasIvica PuljakToni SculacZeljko AntunovicMarko KovacVuko BrigljevicDinko FerencekDevdatta MajumderBenjamin MesicMatej RoguljicAndrei StarodumovTatjana SusaMohsan Waseem AtherAlexandros AttikisEleni ErodotouAimilios IoannouGouranga KoleMarina KolosovaSotiroulla KonstantinouGeorgios MavromanolakisJehad MousaCharalambos NicolaouFotios PtochosPanos A RazisHans RykaczewskiHalil SakaDemetra TsiakkouriMiroslav FingerMichael FingerAntonin KvetonJan TomsaEdy AyalaEdgar Carrera JarrinHassan AbdallaYasser AssranAmr MohamedMohammed MahmoudYasser MohammedSandeep BhowmikAlexandra Carvalho Antunes de OliveiraRam Krishna DewanjeeKarl EhatahtMario KadastikMartti RaidalChristian VeelkenPaula EerolaLaurent ForthommeHenning KirschenmannKenneth OsterbergMikko VoutilainenErik BrückenFrancisco Ignacio Garcia FuentesJoona HavukainenVeikko KarimäkiMin Suk KimRitva KinnunenTapio LampénKati Lassila-PeriniSanteri LaurilaSami LehtiTomas LindénHannu SiikonenEija TuominenJorma TuominiemiPanja-Riina LuukkaTuure TuuvaChiara AmendolaMarc BesanconFabrice CoudercMarc DejardinDaniel DenegriJean-Louis FaureFederico FerriSerguei GanjourAlain GivernaudPhilippe GrasGautier Hamel de MonchenaultPatrick JarryBruno LenziElizabeth LocciJulie MalclesJohn RanderAndré RosowskyMehmet Özgür SahinAurore Savoy-NavarroMaksym TitovGeum Bong YuSudha AhujaFlorian BeaudetteMatteo BonanomiAxel Buchot PerraguinPhilippe BussonClaude CharlotOlivier DavignonBatoul DiabGuillaume FalmagneRaphael Granier de CassagnacAlexandre HakimiInna KucherArtur LobanovCristina Martin PerezMatthew NguyenChristophe OchandoPascal PaganiniJonas RembserRoberto SalernoJean-Baptiste SauvanYves SiroisAlexandre ZabiAmina ZghicheJean-Laurent AgramJeremy AndreaDaniel BlochGuillaume BourgatteJean-Marie BromEric Christian ChabertCaroline CollardJean-Charles FontaineDenis GeléUlrich GoerlachClément GrimaultAnne-Catherine Le BihanPierre van HoveEce AsilarStephanie BeauceronColin BernetGaelle BoudoulCamille CamenAurélien CarleNicolas ChanonDidier ContardoPierre DepasseHoumani El MamouniJean FaySusan GasconMaxime GouzevitchBernard IlleSandhya JainImad Baptiste LaktinehHugues LattaudAntoine LesauvageMorgan LethuillierLaurent MirabitoLucas TorterototGaël TouquetMuriel Vander DoncktSébastien ViretTengizi ToriashviliZviad TsamalaidzeLutz FeldKatja KleinMartin LipinskiDanilo MeuserAlexander PaulsMarius PreutenMax Philip RauchJohannes SchulzMarius TeroerdeDmitry EliseevMartin ErdmannPeter FackeldeyBenjamin FischerSaranya GhoshThomas HebbekerKerstin HoepfnerHenning KellerLuca MastrolorenzoMarkus MerschmeyerArnd MeyerPhilipp MilletGiovanni MocellinSpandan MondalSwagata MukherjeeDennis NollAndrzej NovakTobias PookAndrey PozdnyakovThorben QuastMarkus RadziejYannik RathHans ReithlerJonas 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HusemannKonstantinos KousourisIoannis PapakrivopoulosGeorgios TsipolitisAnna ZacharopoulouIoannis EvangelouCostas FoudasParaskevas GianneiosPanagiotis KatsoulisPanagiotis KokkasStavros MalliosKalliopi ManitaraNikolaos ManthosIoannis PapadopoulosJohn StrologasMárton BartókRuchi ChudasamaMate CsanadMahmod Moussa Abdelkhalek GadallahSándor LökösPéter MajorKoushik MandalAnkita MehtaGabriella PasztorOlivér SurányiGabor Istvan VeresGyorgy BenczeCsaba HajduDezso HorvathFerenc SiklerViktor VeszpremiGyorgy VesztergombiSandor CzellarJános KarancsiJozsef MolnarZoltan SzillasiDaniel TeyssierPeter RaicsZoltan Laszlo TrocsanyiBalazs UjvariTamas Ferenc CsorgoFrigyes NemesTamas NovakSomnath ChoudhuryJyothsna Rani KomaragiriDeepak KumarLata PanwarPraveen Chandra TiwariSeema BahinipatiDipika DashChandiprasad KarProlay MalTribeni MishraVinaya Krishnan Muraleedharan Nair BindhuAruna NayakDeepak Kumar SahooNairit SurSanjay Kumar SwainSunil BansalSuman Bala BeriVipin BhatnagarSushil ChauhanNitish 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FanfaniElisa FontanesiPaolo GiacomelliLuca GiommiClaudio GrandiLuigi GuiducciFabio IemmiSergio Lo MeoStefano MarcelliniGianni MasettiFrancesco NavarriaAndrea PerrottaFederica PrimaveraTiziano RovelliGian Piero SiroliNicolò TosiSebastiano AlbergoSalvatore CostaAlessandro Di MattiaRenato PotenzaAlessia TricomiCristina TuveGiuseppe BarbagliAntonio CasseseRudy CeccarelliVitaliano CiulliCarlo CivininiRaffaello d'AlessandroFrancesco FioriEttore FocardiGiuseppe LatinoPiergiulio LenziMattia LizzoMarco MeschiniSimone PaolettiRoberto SeiditaGiacomo SguazzoniLorenzo VilianiLuigi BenussiStefano BiancoDavide PiccoloMarco BozzoFabrizio FerroRoberto MulargiaEnrico RobuttiSilvano TosiAndrea BenagliaAndrea BeschiFrancesco BrivioFlavia CetorelliVincenzo CirioloFederico de GuioMauro Emanuele DinardoPaolo DiniSimone GennaiAlessio GhezziPietro GovoniLuca GuzziMartina MalbertiSandra MalvezziDario MenasceFabio MontiLuigi MoroniMarco PaganoniDaniele PedriniStefano RagazziTommaso Tabarelli de FatisDavide ValsecchiDavide ZuoloSalvatore BuontempoNicola CavalloAgostino de IorioFrancesco FabozziFrancesco FiengaAlberto Orso Maria IorioLukas LayerLuca ListaSabino MeolaPierluigi PaolucciBiagio RossiCrisostomo SciaccaElena VoevodinaPatrizia AzziNicola BacchettaDario BiselloAlessio BolettiAlberto BragagnoloRoberto CarlinPaolo ChecchiaPablo de Castro ManzanoTommaso DorigoFabrizio GaspariniUgo GaspariniSiew Yan HohMartino MargoniAnna Teresa MeneguzzoMatteo PresillaPaolo RoncheseRoberto RossinFranco SimonettoGiles StrongAndres TikoMia TosiHevjin YararMarco ZanettiPierluigi ZottoAlberto ZucchettaAlessandro BraghieriSimone CalzaferriDavide FiorinaPaolo MontagnaSergio P RattiValerio ReMartina RessegottiCristina RiccardiPaola SalviniIlaria VaiPaolo VituloMaurizio BiasiniGian Mario BileiDiego CiangottiniLivio FanòPaolo LaricciaGiancarlo MantovaniValentina MarianiMauro MenichelliFrancesco MoscatelliAlessandro RossiAttilio SantocchiaDaniele SpigaTommaso TedeschiKonstantin AndrosovPaolo AzzurriGiuseppe 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• Publié dans Eur.Phys.J.C le 30/10/2025

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Résumé : This paper presents new sets of parameters (“tunes”) for the underlying-event model of the ${\textsc {herwig}} \,7$ event generator. These parameters control the description of multiple-parton interactions (MPI) and colour reconnection in ${\textsc {herwig}} \,7$, and are obtained from a fit to minimum-bias data collected by the CMS experiment at $\sqrt{s}=0.9$, 7, and $13 \,\text {Te}\text {V} $. The tunes are based on the NNPDF 3.1 next-to-next-to-leading-order parton distribution function (PDF) set for the parton shower, and either a leading-order or next-to-next-to-leading-order PDF set for the simulation of MPI and the beam remnants. Predictions utilizing the tunes are produced for event shape observables in electron-positron collisions, and for minimum-bias, inclusive jet, top quark pair, and Z and W boson events in proton-proton collisions, and are compared with data. Each of the new tunes describes the data at a reasonable level, and the tunes using a leading-order PDF for the simulation of MPI provide the best description of the data.

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Fichiers liés : hal-03022767.pdf

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Source

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• Type de publi. : Article dans une revue
• Date de publi. : 01/01/2021
• Auteurs : Albert M SirunyanArmen TumasyanWolfgang AdamThomas BergauerMarko DragicevicJanos EröAlberto Escalante del ValleRudolf FruehwirthManfred JeitlerNatascha KrammerLukas LechnerDietrich LikoThomas MadlenerIvan MikulecFlorian Michael PittersNavid RadJochen SchieckRobert SchöfbeckMarkus SpanringSebastian TemplWolfgang WaltenbergerClaudia-Elisabeth WulzMateusz ZaruckiVladimir ChekhovskyAliaksandr LitominVladimir MakarenkoJuan Suarez GonzalezMohamed Rashad DarwishEddi A de WolfDavide Di CroceXavier JanssenTomas KelloAleksandra LelekMaxim PietersHaifa Rejeb SfarHans van HaevermaetPierre van MechelenSenne van PutteNick van RemortelFreya BlekmanEmil Sørensen BolsSimranjit Singh ChhibraJorgen d'HondtJarne de ClercqDenys LontkovskyiSteven LowetteIvan MarchesiniSeth MoortgatAlexander MortonQuentin PythonStefaan TavernierWalter van DoninckPetra van MuldersDiego BeghinBugra BilinBarbara ClerbauxGilles de LentdeckerBrian DorneyLaurent FavartAnastasia GrebenyukAmandeep Kaur KalsiInna MakarenkoLouis MoureauxLaurent PétréAndrey PopovNicolas PostiauElizabeth StarlingLaurent ThomasCatherine Vander VeldePascal VanlaerDavid VanneromLiam WezenbeekTom CornelisDidar DoburMarek GruchalaIllia KhvastunovMarek NiedzielaChristos RoskasKirill SkovpenMichael TytgatWillem VerbekeBasile VermassenMartina VitGiacomo BrunoFlorian Joel J BuryClaudio CaputoPieter DavidChristophe DelaereMartin DelcourtIzzeddin Suat DonertasAndrea GiammancoVincent LemaitreKuntal MondalJessica PrisciandaroAngela TaliercioMaksym TeklishynPietro VischiaSébastien WertzSophie WuyckensGilvan AlvesCarsten HenselArthur MoraesWalter Luiz Aldá JúniorEwerton Belchior Batista das ChagasHelena Brandao MalbouissonWagner CarvalhoJose ChinellatoEduardo CoelhoEliza Melo da CostaGustavo Gil da SilveiraDilson de Jesus DamiaoSandro Fonseca de SouzaJordan MartinsDiego Matos FigueiredoMiguel Medina JaimeClemencia Mora HerreraLuiz MundimHelio NogimaPatricia Rebello TelesLuis Sanchez RosasAlberto SantoroSheila Mara Silva Do AmaralAndre SznajderMauricio ThielFelipe Torres da Silva de AraujoAntonio Vilela PereiraCesar Augusto BernardesLuigi CalligarisThiago TomeiEduardo de Moraes GregoresDener de Souza LemosPedro G MercadanteSergio F NovaesSandra PadulaAleksandar AleksandrovGeorgy AntchevIvan AtanasovRoumyana HadjiiskaPlamen IaydjievMilena MishevaMircho RodozovMariana ShopovaGeorgi SultanovMiroslav BonchevAnton DimitrovTodor IvanovLeander LitovBorislav PavlovPeicho PetkovAnton PetrovWenxing FangQianying GuoHanwen WangLi YuanMuhammad AhmadZhen HuYi WangEmilien ChaponGuo-Ming ChenHe-Sheng ChenMingshui ChenTahir JavaidAnshul KapoorDuncan LeggatHongbo LiaoZhenan LiuRamkrishna SharmaAniello SpieziaJunquan TaoJoshuha Thomas-WilskerJin WangHuaqiao ZhangSijing ZhangJingzhou ZhaoAntonis AgapitosYong BanCheng ChenQianming HuangAndrew LevinQiang LiMeng LuXudong LyuYajun MaoSi-Jin QianDayong WangQun WangJie XiaoZhengyun YouXuyang GaoMeng XiaoCarlos AvilaAndrés CabreraCarlos FlorezJorge FragaAmal SarkarManuel Alejandro 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• Publié dans JHEP le 14/01/2026

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Résumé : Measurements are presented of differential cross sections for the production of Z bosons in association with at least one jet initiated by a charm quark in pp collisions at $ \sqrt{s} $ = 13 TeV. The data recorded by the CMS experiment at the LHC correspond to an integrated luminosity of 35.9 fb$^{−1}$. The final states contain a pair of electrons or muons that are the decay products of a Z boson, and a jet consistent with being initiated by a charm quark produced in the hard interaction. Differential cross sections as a function of the transverse momentum p$_{T}$ of the Z boson and p$_{T}$ of the charm jet are compared with predictions from Monte Carlo event generators. The inclusive production cross section 405.4 ± 5.6 (stat) ± 24.3 (exp) ± 3.7 (theo) pb, is measured in a fiducial region requiring both leptons to have pseudorapidity |η| < 2.4 and p$_{T}$> 10 GeV, at least one lepton with p$_{T}$> 26 GeV, and a mass of the pair in the range 71–111 GeV, while the charm jet is required to have p$_{T}$> 30 GeV and |η| < 2.4. These are the first measurements of these cross sections in proton-proton collisions at 13 TeV.[graphic not available: see fulltext]

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Fichiers liés : Sirunyan2021_Article_MeasurementOfDifferentialCross.pdf

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