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Measurements of WW and WZ production in W + jets final states in pp collisions
Authors:Abazov V M  Abbott B  Acharya B S  Adams M  Adams T  Alexeev G D  Alkhazov G  Alton A  Alverson G  Alves G A  Aoki M  Askew A  Åsman B  Atkins S  Atramentov O  Augsten K  Avila C  BackusMayes J  Badaud F  Bagby L  Baldin B  Bandurin D V  Banerjee S  Barberis E  Baringer P  Barreto J  Bartlett J F  Bassler U  Bazterra V  Bean A  Begalli M  Belanger-Champagne C  Bellantoni L  Beri S B  Bernardi G  Bernhard R  Bertram I  Besançon M  Beuselinck R  Bezzubov V A  Bhat P C  Bhatnagar V  Blazey G  Blessing S  Bloom K  Boehnlein A  Boline D  Boos E E  Borissov G  Bose T  Brandt A  Brandt O  Brock R  Brooijmans G  Bross A  Brown D  Brown J  Bu X B  Buehler M
Institution:Joint Institute for Nuclear Research, Dubna, Russia.
Abstract:We study WW and WZ production with ?νqq (?=e,μ) final states using data collected by the D0 detector at the Fermilab Tevatron Collider corresponding to 4.3 fb(-1) of integrated luminosity from pp collisions at sqrts]=1.96 TeV. Assuming the ratio between the production cross sections σ(WW) and σ(WZ) as predicted by the standard model, we measure the total WV (V=W,Z) cross section to be σ(WV)=19.6(-3.0)(+3.2) pb and reject the background-only hypothesis at a level of 7.9 standard deviations. We also use b-jet discrimination to separate the WZ component from the dominant WW component. Simultaneously fitting WW and WZ contributions, we measure σ(WW)=15.9(-3.2)(+3.7) pb and σ(WZ)=3.3(-3.3)(+4.1) pb, which is consistent with the standard model predictions.
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