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Inclusive b-jet production in pp collisions at √s = 7 TeVChatrchyan, S.Khachatryan, V.Sirunyan, A.M.Tumasyan, A.Adam, W.Bergauer, T.Dragicevic, M.Erö, J.Fabjan, C.Friedl, M.Frühwirth, R.Ghete, V.M.Hammer, J.Hoch, M.Hörmann, N.Hrubec, J.Jeitler, M.Kiesenhofer, W.Krammer, M.Liko, D.Mikulec, I.Pernicka, M.Rahbaran, B.Rohringer, C.Rohringer, H.Schöfbeck, R.Strauss, J.Taurok, A.Teischinger, F.Wagner, P.Waltenberger, W.Walzel, G.Widl, E.Wulz, C.-E.Mossolov, V.Shumeiko, N.Gonzalez, J. SuarezBansal, S.Benucci, L.Cornelis, T.De Wolf, E.A.Janssen, X.Luyckx, S.Maes, T.Mucibello, L.Ochesanu, S.Roland, B.Rougny, R.Selvaggi, M.Van Haevermaet, H.Hadron-Hadron scatteringThe inclusive b-jet production cross section in pp collisions at a center-ofmass energy of 7TeV is measured using data collected by the CMS experiment at the LHC. The cross section is presented as a function of the jet transverse momentum in the range 18 < pT < 200 GeV for several rapidity intervals. The results are also given as the ratio of the b-jet production cross section to the inclusive jet production cross section. The measurement is performed with two different analyses, which differ in their trigger selection and b-jet identification: a jet analysis that selects events with a b jet using a sample corresponding to an integrated luminosity of 34 pb-1, and a muon analysis requiring a b jet with a muon based on an integrated luminosity of 3 pb-1. In both approaches the b jets are identified by requiring a secondary vertex. The results from the two methods are in agreement with each other and with next-to-leading order calculations, as well as with predictions based on the pythia event generator.2012Articlehttps://rdlopen.rawdatalibrary.net/r/ebyu/15751https://doi.org/10.1007/jhep04(2012)0841126-6708enJournal of High Energy Physicsinfo:eu-repo/semantics/openAccessinfo:eu-repo/semantics/articlehttps://ebyu-rdlopen.rawdatalibrary.net/tr/items/ebyu/15751