Evidence for s-channel single top quark production in pp¯ collisions at s=1.96 TeV

We present measurements of the cross sections for the two main production modes of single top quarks in pp¯ collisions at s=1.96 TeV in the Run II data collected with the D0 detector at the Fermilab Tevatron Collider, corresponding to an integrated luminosity of 9.7 fb−1. The s-channel cross section...

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Veröffentlicht in:Physics letters. B 2013-11, Vol.726 (4-5), p.656-664
Hauptverfasser: Abbott, B., Adams, M., Adams, T., Alexeev, G.D., Alton, A., Askew, A., Avila, C., Barberis, E., Baringer, P., Bartlett, J.F., Bazterra, V., Bean, A., Bernhard, R., Boehnlein, A., Boline, D., Borissov, G., Brock, R., Casey, B.C.K., Chan, K.M., Chandra, A., Choi, S., Choudhary, B., Cihangir, S., Clutter, J., Couderc, F., Cousinou, M.-C., Denisov, D., Deterre, C., Diehl, H.T., Dominguez, A., Dubey, A., Elvira, V.D., Fisher, W., Fisk, H.E., Fortner, M., Fuess, S., Garcia-Bellido, A., Gershtein, Y., Ginther, G., Grünendahl, S., Hebbeker, T., Herner, K., Hesketh, G., Hoang, T., Hogan, J., Hubacek, Z., Ito, A.S., Jayasinghe, A., Jeong, M.S., Johnson, E., Karmanov, D., Kehoe, R., Kermiche, S., Kharzheev, Y.N., Kraus, J., Kurča, T., Kuzmin, V.A., Lim, J.K., Linnemann, J., Lipaev, V.V., Madar, R., Meyer, A., Meyer, J., Miconi, F., Mondal, N.K., Nagy, E., Osman, N., Pal, A., Parashar, N., Parua, N., Patwa, A., Peters, Y., Prewitt, M., Prokopenko, N., Quadt, A., Ratoff, P.N., Rominsky, M., Royon, C., Sajot, G., Scanlon, T., Scheglov, Y., Schellman, H., Shary, V., Simak, V., Slattery, P., Smirnov, D., Snyder, S., Stoyanova, D.A., Tully, C., Vasilyev, I.A., Wayne, M., Williams, M.R.J., Wood, D.R., Xie, Y., Yamada, R., Ye, Z., Yin, H., Yu, J.M., Zhao, T.G., Zieminska, D.
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Sprache:eng
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Zusammenfassung:We present measurements of the cross sections for the two main production modes of single top quarks in pp¯ collisions at s=1.96 TeV in the Run II data collected with the D0 detector at the Fermilab Tevatron Collider, corresponding to an integrated luminosity of 9.7 fb−1. The s-channel cross section is measured to be σ(pp¯→tb+X)=1.10−0.31+0.33 pb with no assumptions on the value of the t-channel cross section. Similarly, the t-channel cross section is measured to be σ(pp¯→tqb+X)=3.07−0.49+0.54 pb. We also measure the s+t combined cross section as σ(pp¯→tb+X,tqb+X)=4.11−0.55+0.60 pb and set a lower limit on the CKM matrix element |Vtb|>0.92 at 95% C.L., assuming mt=172.5 GeV. The probability to measure a cross section for the s channel at the observed value or higher in the absence of signal is 1.0×10−4, corresponding to a significance of 3.7 standard deviations.
ISSN:0370-2693
1873-2445
DOI:10.1016/j.physletb.2013.09.048