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We present a measurement of the ttbar production cross section multiplied by the branching ratio to tau lepton decaying semihadronically plus jets, at a center of mass energy sqrt{s}=1.96 TeV using 1 fb^(-1) of integrated luminosity collected with the D0 detector.
V. Barger and R.J.N. Phillips, Phys. Rev. D 41
1990
Earlier work this paper cites.
S. Jadach, Z. Was, R. Decker, and J.H. Kuehn, Comp. Phys. Commun. 76
1993
Earlier work this paper cites.
R. Brun and F. Carminati, CERN Program Library Long Writeup W5013 (unpublished), (1993)
1993
Earlier work this paper cites.
J. Guasch and J. Sola, Phys. Lett. B 416
1998
Earlier work this paper cites.
T. Han and M.B. Magro, Phys. Lett. B 476
2000
Earlier work this paper cites.
G.C. Blazey et al
2000
Earlier work this paper cites.
T. Sjöstrand et al
2001
Earlier work this paper cites.
D.J. Lange, Nucl. Instrum. Methods Phys. Res. A 462
2001
Earlier work this paper cites.
C. Yue, H. Zong and L. Liu, Mod. Phys. Lett. 18
2003
Earlier work this paper cites.
M.L. Mangano et al
2003
Cited alongside, same era.
J. Pumplin et al
2003
Cited alongside, same era.
A. Schwartzman, Report No. FERMILAB-THESIS-2004-2
2004
Cited alongside, same era.
S. Höche et al
2004
Cited alongside, same era.
V.M. Abazov et al
2006
Cited alongside, same era.
A. Abulencia et al
2006
Cited alongside, same era.
V.M. Abazov et al
2007
Cited alongside, same era.
V.M. Abazov et al
2007
Cited alongside, same era.
M. Cacciari et al
2008
Later among the works it cites.
N. Kidonakis and R. Vogt, Phys. Rev. D 78
2008
Later among the works it cites.
S. Moch and P. Uwer, Phys. Rev. D 78
2008
Later among the works it cites.
C. Amsler et al
2008
Later among the works it cites.
V.M. Abazov et al
2009
Later among the works it cites.
J. Hegeman, J. Phys. Conf. Ser. 160
2009
Later among the works it cites.
V.M. Abazov et al
2009
Later among the works it cites.
V.M. Abazov et al
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T. Andeen et al
2007
Cited alongside, same era.
The D0 coordinate system has the positive z z -axis along the proton beamline, and z = 0 z=0 at the center of the detector. The polar and azimuthal angles are denoted as θ \theta and ϕ \phi , respectively. The pseudorapidity is defined as η = − ln ( tan θ 2 ) \eta=-\ln(\tan\frac{\theta}{2})
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The aplanarity is 3 / 2 λ 3 3/2\lambda_{3} , with λ 3 \lambda_{3} being the smallest eigenvalue of the momentum tensor M α β = ∑ i p i α p i β / ∑ i | p → i | 2 M^{\alpha\beta}=\sum_{i}p_{i}^{\alpha}p_{i}^{\beta}/\sum_{i}|\vec{p}_{i}|^{2} , where i i runs over the number of jets and the τ \tau lepton candidate, and α , β = 1 , 2 , 3 \alpha,\beta=1,2,3 specifies the three spatial components of the momentum
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2010
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V.M. Abazov et al
2010
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