Login / Signup

High-precision measurement of the W boson mass with the CDF II detector.

null nullT AaltonenS AmerioD AmideiA AnastassovA AnnoviJ AntosG ApollinariJ A AppelT ArisawaA ArtikovJ AsaadiW AshmanskasB AuerbachA AurisanoF AzfarW BadgettT BaeA Barbaro-GaltieriV E BarnesB A BarnettP BarriaP BartosM BauceF BedeschiS BehariG BellettiniJ BellingerD BenjaminA BeretvasA BhattiK R BlandB BlumenfeldA BocciA BodekD BortolettoJ BoudreauA BoveiaL BrigliadoriC BrombergE BruckenJ BudagovH S BuddK BurkettG BusettoP BusseyP ButtiA BuzatuA CalambaS CamardaM CampanelliB CarlsD CarlsmithR CarosiS CarrilloB CasalM CasarsaA CastroP CatastiniD CauzV CavaliereA CerriL CerritoY C ChenM ChertokG ChiarelliG ChlachidzeKihyeon ChoD ChokheliA ClarkC ClarkeM E ConveryJ ConwayM CorboM CordelliC A CoxD J CoxM CremonesiD CruzJ CuevasR CulbertsonN d'AscenzoM DattaP de BarbaroL DemortierM DeninnoM D'ErricoF DevotoA Di CantoB Di RuzzaJ R DittmannS DonatiM D'OnofrioM DorigoA DriuttiK EbinaR EdgarA ElaginR ErbacherS ErredeB EshamS FarringtonJ P Fernández RamosR FieldG FlanaganR ForrestM FranklinJ C FreemanH FrischY FunakoshiC GalloniA F GarfinkelP GarosiH GerberichE GerchteinS GiaguV GiakoumopoulouK GibsonC M GinsburgN GiokarisP GirominiV GlagolevD GlenzinskiM GoldD GoldinA GolossanovG GomezG Gomez-CeballosM GoncharovO González LópezI GorelovA T GoshawK GoulianosE GramelliniC Grosso-PilcherJ Guimaraes da CostaS R HahnJ Y HanF HappacherK HaraM HareR F HarrT Harrington-TaberK HatakeyamaC HaysJ HeinrichM HerndonA HockerZiqing HongW HopkinsS HouR E HughesU HusemannM HusseinJ HustonG IntrozziM IoriA IvanovE JamesD JangB JayatilakaE J JeonS JindarianiM JonesK K JooS Y JunT R JunkM KambeitzT KamonP E KarchinA KasmiY KatoW KetchumJ KeungB KilminsterD H KimH S KimJ E KimM J KimS H KimS B KimY J KimY K KimN KimuraM KirbyK KondoD J KongJ KonigsbergA V KotwalM KrepsJ KrollM KruseT KuhrM KurataA T LaasanenS LammelM LancasterK LannonG LatinoHyun Su LeeJ S LeeS LeoS LeoneJ D LewisA LimosaniE LipelesA ListerQ LiuT LiuS LockwitzA LoginovD LucchesiA LucàJ LueckP LujanP LukensG LunguJ LysR LysakR MadrakP MaestroS MalikG MancaA Manousakis-KatsikakisL MarcheseF MargaroliP MarinoK MateraM E MattsonA MazzacaneP MazzantiR McNultyA MehtaP MehtalaA MenzioneC MesropianT MiaoE MichielinD MietlickiA MitraH MiyakeS MoedN MoggiC S MoonR MooreM J MorelloA MukherjeeTh MullerP MuratM MussiniJ NachtmanY NagaiJ NaganomaI NakanoA NapierJ NettT NigmanovL NodulmanS Y NohO NorniellaL OakesS H OhY D OhT OkusawaR OravaL OrtolanC PagliaroneE PalenciaP PalniV PapadimitriouW ParkerG PaulettaM PauliniC PausT J PhillipsG PiacentinoE PianoriJ PilotK PittsC PlagerL PondromS PoprockiK PotamianosA PrankoF ProkoshinF PtochosG PunziI Redondo FernándezP RentonM RescignoF RimondiL RistoriA RobsonT RodriguezS RolliM RonzaniR RoserJ L RosnerF RuffiniA RuizJ RussV RusuW K SakumotoY SakuraiL SantiK SatoV SavelievA Savoy-NavarroP SchlabachE E SchmidtT SchwarzL ScodellaroF ScuriSally SeidelY SeiyaA SemenovF SforzaS Z ShalhoutT ShearsP F ShepardM ShimojimaM ShochetI Shreyber-TeckerA SimonenkoK SliwaJ R SmithF D SniderH SongV SorinR St DenisM StancariD StentzJ StrologasY SudoA SukhanovI SuslovK TakemasaY TakeuchiJ TangM TecchioP K TengJ ThomE ThomsonV ThukralD TobackS TokarK TollefsonT TomuraS TorreD TorrettaP TotaroM TrovatoF UkegawaS UozumiF VázquezG VelevCostas VellidisC VernieriM VidalR VilarJ VizánM VogelG VolpiP WagnerR WallnyS M WangD WatersW C WesterD WhitesonA B WicklundS WilburH H WilliamsJ S WilsonP WilsonB L WinerP WittichS WolbersH WolfmeisterT WrightX WuZ WuK YamamotoD YamatoT YangU K YangY C YangW-M YaoG P YehK YiJ YohK YoritaT YoshidaG B YuI YuA M ZanettiY ZengC ZhouS Zucchelli
Published in: Science (New York, N.Y.) (2022)
The mass of the W boson, a mediator of the weak force between elementary particles, is tightly constrained by the symmetries of the standard model of particle physics. The Higgs boson was the last missing component of the model. After observation of the Higgs boson, a measurement of the W boson mass provides a stringent test of the model. We measure the W boson mass, M W , using data corresponding to 8.8 inverse femtobarns of integrated luminosity collected in proton-antiproton collisions at a 1.96 tera-electron volt center-of-mass energy with the CDF II detector at the Fermilab Tevatron collider. A sample of approximately 4 million W boson candidates is used to obtain [Formula: see text] , the precision of which exceeds that of all previous measurements combined (stat, statistical uncertainty; syst, systematic uncertainty; MeV, mega-electron volts; c , speed of light in a vacuum). This measurement is in significant tension with the standard model expectation.
Keyphrases
  • computed tomography
  • magnetic resonance imaging
  • cell proliferation
  • preterm infants
  • single molecule
  • deep learning
  • smoking cessation
  • electronic health record
  • image quality
  • data analysis
  • preterm birth