A first measurement of the polarization of W bosons with large transverse momenta in pp collisions is presented. The measurement is based on 36 pb⁻¹ of data recorded at √s = 7 TeV by the CMS detector at the LHC. The left-handed, right-handed, and longitudinal polarization fractions (f(L), f(R), and f₀, respectively) of W bosons with transverse momenta larger than 50 GeV are determined by using decays to both electrons and muons. The muon final state yields the most precise measurement: (f(L) - f(R))⁻ = 0.240 ± 0.036(stat) ± 0.031(syst) and f₀⁻ = 0.183 ± 0.087(stat) ± 0.123(syst) for negatively charged W bosons and (f(L) - f(R))⁺ = 0.310 ± 0.036(stat) ± 0.017(syst) and f₀⁺ = 0.171 ± 0.085(stat) ± 0.099(syst) for positively charged W bosons. This establishes, for the first time, that W bosons produced in pp collisions with large transverse momenta are predominantly left-handed, as expected in the standard model.
A first measurement of the polarization of W bosons with large transverse momenta in pp collisions is presented. The measurement is based on 36 pb⁻¹ of data recorded at √s = 7 TeV by the CMS detector at the LHC. The left-handed, right-handed, and longitudinal polarization fractions (f(L), f(R), and f₀, respectively) of W bosons with transverse momenta larger than 50 GeV are determined by using decays to both electrons and muons. The muon final state yields the most precise measurement: (f(L) - f(R))⁻ = 0.240 ± 0.036(stat) ± 0.031(syst) and f₀⁻ = 0.183 ± 0.087(stat) ± 0.123(syst) for negatively charged W bosons and (f(L) - f(R))⁺ = 0.310 ± 0.036(stat) ± 0.017(syst) and f₀⁺ = 0.171 ± 0.085(stat) ± 0.099(syst) for positively charged W bosons. This establishes, for the first time, that W bosons produced in pp collisions with large transverse momenta are predominantly left-handed, as expected in the standard model.
Authors: G Aad; T Abajyan; B Abbott; J Abdallah; S Abdel Khalek; A A Abdelalim; O Abdinov; R Aben; B Abi; M Abolins; O S AbouZeid; H Abramowicz; H Abreu; B S Acharya; L Adamczyk; D L Adams; T N Addy; J Adelman; S Adomeit; P Adragna; T Adye; S Aefsky; J A Aguilar-Saavedra; M Agustoni; S P Ahlen; F Ahles; A Ahmad; M Ahsan; G Aielli; T P A Åkesson; G Akimoto; A V Akimov; M A Alam; J Albert; S Albrand; M Aleksa; I N Aleksandrov; F Alessandria; C Alexa; G Alexander; G Alexandre; T Alexopoulos; M Alhroob; M Aliev; G Alimonti; J Alison; B M M Allbrooke; L J Allison; P P Allport; S E Allwood-Spiers; J Almond; A Aloisio; R Alon; A Alonso; F Alonso; A Altheimer; B Alvarez Gonzalez; M G Alviggi; K Amako; C Amelung; V V Ammosov; S P Amor Dos Santos; A Amorim; S Amoroso; N Amram; C Anastopoulos; L S Ancu; N Andari; T Andeen; C F Anders; G Anders; K J Anderson; A Andreazza; V Andrei; X S Anduaga; S Angelidakis; P Anger; A Angerami; F Anghinolfi; A Anisenkov; N Anjos; A Annovi; A Antonaki; M Antonelli; A Antonov; J Antos; F Anulli; M Aoki; L Aperio Bella; R Apolle; G Arabidze; I Aracena; Y Arai; A T H Arce; S Arfaoui; J-F Arguin; S Argyropoulos; E Arik; M Arik; A J Armbruster; O Arnaez; V Arnal; A Artamonov; G Artoni; D Arutinov; S Asai; S Ask; B Åsman; L Asquith; K Assamagan; R Astalos; A Astbury; M Atkinson; B Auerbach; E Auge; K Augsten; M Aurousseau; G Avolio; D Axen; G Azuelos; Y Azuma; M A Baak; G Baccaglioni; C Bacci; A M Bach; H Bachacou; K Bachas; M Backes; M Backhaus; J Backus Mayes; E Badescu; P Bagnaia; Y Bai; D C Bailey; T Bain; J T Baines; O K Baker; S Baker; P Balek; F Balli; E Banas; P Banerjee; Sw Banerjee; D Banfi; A Bangert; V Bansal; H S Bansil; L Barak; S P Baranov; T Barber; E L Barberio; D Barberis; M Barbero; D Y Bardin; T Barillari; M Barisonzi; T Barklow; N Barlow; B M Barnett; R M Barnett; A Baroncelli; G Barone; A J Barr; F Barreiro; J Barreiro Guimarães da Costa; R Bartoldus; A E Barton; V Bartsch; A Basye; R L Bates; L Batkova; J R Batley; A Battaglia; M Battistin; 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W Willis; S Willocq; J A Wilson; M G Wilson; A Wilson; I Wingerter-Seez; S Winkelmann; F Winklmeier; M Wittgen; T Wittig; J Wittkowski; S J Wollstadt; M W Wolter; H Wolters; W C Wong; G Wooden; B K Wosiek; J Wotschack; M J Woudstra; K W Wozniak; K Wraight; M Wright; B Wrona; S L Wu; X Wu; Y Wu; E Wulf; B M Wynne; S Xella; M Xiao; S Xie; C Xu; D Xu; L Xu; B Yabsley; S Yacoob; M Yamada; H Yamaguchi; Y Yamaguchi; A Yamamoto; K Yamamoto; S Yamamoto; T Yamamura; T Yamanaka; K Yamauchi; T Yamazaki; Y Yamazaki; Z Yan; H Yang; H Yang; U K Yang; Y Yang; Z Yang; S Yanush; L Yao; Y Yasu; E Yatsenko; J Ye; S Ye; A L Yen; M Yilmaz; R Yoosoofmiya; K Yorita; R Yoshida; K Yoshihara; C Young; C J S Young; S Youssef; D Yu; D R Yu; J Yu; J Yu; L Yuan; A Yurkewicz; B Zabinski; R Zaidan; A M Zaitsev; S Zambito; L Zanello; D Zanzi; A Zaytsev; C Zeitnitz; M Zeman; A Zemla; O Zenin; T Ženiš; D Zerwas; G Zevi Della Porta; D Zhang; H Zhang; J Zhang; L Zhang; X Zhang; Z Zhang; L Zhao; Z Zhao; A Zhemchugov; J Zhong; B Zhou; N Zhou; Y Zhou; C G Zhu; H Zhu; J Zhu; Y Zhu; X Zhuang; V Zhuravlov; A Zibell; D Zieminska; N I Zimin; R Zimmermann; S Zimmermann; S Zimmermann; Z Zinonos; M Ziolkowski; R Zitoun; L Živković; V V Zmouchko; G Zobernig; A Zoccoli; M Zur Nedden; V Zutshi; L Zwalinski Journal: Eur Phys J C Part Fields Date: 2013-05-15 Impact factor: 4.590
Authors: S Chatrchyan; V Khachatryan; A M Sirunyan; A Tumasyan; W Adam; E Aguilo; T Bergauer; M Dragicevic; J Erö; C Fabjan; M Friedl; R Frühwirth; V M Ghete; J Hammer; N Hörmann; J Hrubec; M Jeitler; W Kiesenhofer; V Knünz; M Krammer; I Krätschmer; D Liko; I Mikulec; M Pernicka; B Rahbaran; C Rohringer; H Rohringer; R Schöfbeck; J Strauss; A Taurok; W Waltenberger; G Walzel; E Widl; C-E Wulz; V Mossolov; N Shumeiko; J Suarez Gonzalez; M Bansal; S Bansal; T Cornelis; E A De Wolf; X Janssen; S Luyckx; L Mucibello; S Ochesanu; B Roland; R Rougny; M Selvaggi; Z Staykova; H Van Haevermaet; P Van Mechelen; N Van Remortel; A Van Spilbeeck; F Blekman; S Blyweert; J D'Hondt; R Gonzalez Suarez; A Kalogeropoulos; M Maes; A Olbrechts; W Van Doninck; P Van Mulders; G P Van Onsem; I Villella; B Clerbaux; G De Lentdecker; V Dero; A P R Gay; T Hreus; A Léonard; P E Marage; A Mohammadi; T Reis; L Thomas; G Vander Marcken; C Vander Velde; P Vanlaer; J Wang; V Adler; K Beernaert; A Cimmino; S Costantini; G Garcia; M Grunewald; B Klein; J Lellouch; A Marinov; J Mccartin; A A Ocampo Rios; D Ryckbosch; N Strobbe; F Thyssen; M Tytgat; P Verwilligen; S Walsh; E Yazgan; N Zaganidis; S Basegmez; G Bruno; R Castello; L Ceard; C Delaere; T du Pree; D Favart; L Forthomme; A Giammanco; J Hollar; V Lemaitre; J Liao; O Militaru; C Nuttens; D Pagano; A Pin; K Piotrzkowski; N Schul; J M Vizan Garcia; N Beliy; T Caebergs; E Daubie; G H Hammad; G A Alves; M Correa Martins Junior; T Martins; M E Pol; M H G Souza; W L Aldá Júnior; W Carvalho; A Custódio; E M Da Costa; D De Jesus Damiao; C De Oliveira Martins; S Fonseca De Souza; D Matos Figueiredo; L Mundim; H Nogima; W L Prado Da Silva; A Santoro; L Soares Jorge; A Sznajder; T S Anjos; C A Bernardes; F A Dias; T R Fernandez Perez Tomei; E M Gregores; C Lagana; F Marinho; P G Mercadante; S F Novaes; Sandra S Padula; V Genchev; P Iaydjiev; S Piperov; M Rodozov; S Stoykova; G Sultanov; V Tcholakov; R Trayanov; M Vutova; A Dimitrov; R Hadjiiska; V Kozhuharov; 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W Flanagan; J Gilmore; T Kamon; V Khotilovich; R Montalvo; I Osipenkov; Y Pakhotin; A Perloff; J Roe; A Safonov; T Sakuma; S Sengupta; I Suarez; A Tatarinov; D Toback; N Akchurin; J Damgov; C Dragoiu; P R Dudero; C Jeong; K Kovitanggoon; S W Lee; T Libeiro; Y Roh; I Volobouev; E Appelt; A G Delannoy; C Florez; S Greene; A Gurrola; W Johns; P Kurt; C Maguire; A Melo; M Sharma; P Sheldon; B Snook; S Tuo; J Velkovska; M W Arenton; M Balazs; S Boutle; B Cox; B Francis; J Goodell; R Hirosky; A Ledovskoy; C Lin; C Neu; J Wood; S Gollapinni; R Harr; P E Karchin; C Kottachchi Kankanamge Don; P Lamichhane; A Sakharov; M Anderson; D A Belknap; L Borrello; D Carlsmith; M Cepeda; S Dasu; E Friis; L Gray; K S Grogg; M Grothe; R Hall-Wilton; M Herndon; A Hervé; P Klabbers; J Klukas; A Lanaro; C Lazaridis; J Leonard; R Loveless; A Mohapatra; I Ojalvo; F Palmonari; G A Pierro; I Ross; A Savin; W H Smith; J Swanson Journal: Eur Phys J C Part Fields Date: 2013-05-08 Impact factor: 4.590