Fetching the paper…
Reading the bibliography…
We search for annihilation decay modes of neutral $b$ mesons into pairs of charmless charged hadrons with the upgraded Collider Detector at the Fermilab Tevatron.
E. Barberio and Z. Was, Comput. Phys. Commun. 79
1994
Earlier work this paper cites.
G. J. Feldman and R. D. Cousins, Phys. Rev. D 57
1998
Earlier work this paper cites.
C. W. Bauer, S. Fleming and M. Luke, Phys. Rev. D 63
2000
Earlier work this paper cites.
M. Beneke and M. Neubert, Nucl. Phys. B675
2003
Earlier work this paper cites.
J.-F. Sun, G.-H. Zhu, and D.-S. Du, Phys. Rev. D 68
2003
Earlier work this paper cites.
Y. Li, C.-D. Lu, Z.-J. Xiao, and X.-Q. Yu, Phys. Rev. D 70
2004
Earlier work this paper cites.
A. J. Buras, R. Fleischer, S. Recksiegel, and F. Schwab, Nucl. Phys. B697
2004
Earlier work this paper cites.
D. London and J. Matias, Phys. Rev. D 70
2004
Earlier work this paper cites.
D. Acosta et al
2004
Cited alongside, same era.
A. Abulencia et al
2006
Cited alongside, same era.
A. Ali et al
2007
Cited alongside, same era.
A. Soni and D. A. Suprun, Phys. Rev. D 75
2007
Cited alongside, same era.
R. Fleischer, Eur. Phys. J. C 52
2007
Cited alongside, same era.
K. Abe et al
2007
Cited alongside, same era.
M.J. Morello, Ph.D. thesis, Scuola Normale Superiore, Pisa, Fermilab Report No. FERMILAB-THESIS-2007-57 (2007)
2007
Cited alongside, same era.
B. Aubert et al
2007
Later among the works it cites.
H.-Y. Cheng and C.-K. Chua, Phys. Rev. D 80
2009
Later among the works it cites.
T. Aaltonen et al
2009
Later among the works it cites.
K. Nakamura et al
2010
Later among the works it cites.
T. Aaltonen et al
2011
Closest in time.
T. Aaltonen et al
2011
Closest in time.
G. Zhu, Phys. Lett. B 702
2011
Closest in time.
alphaXiv searches the wider corpus for related work and actual follow-ups.
alphaXiv is searching for related work…
Throughout this paper, C-conjugate modes are implied and branching fractions indicate CP-averages
Cited in the paper.
CDF II uses a cylindrical coordinate system in which ϕ \phi is the azimuthal angle, r r is the radius from the nominal beam line, and z z points in the proton beam direction, with the origin at the center of the detector. The transverse plane is the plane perpendicular to the z z axis
Cited in the paper.
Isolation is defined as I B = p T ( B ) / [ p T ( B ) + ∑ i p T i ] I_{B}=p_{T}(B)/[p_{T}(B)+\sum_{i}p_{Ti}] , where p T ( B ) p_{T}(B) is the transverse momentum of the B B candidate, and the sum runs over all other tracks within a cone of radius 1, in η \eta - ϕ \phi space around the B B flight-direction
Cited in the paper.
F. Ruffini, Ph.D. thesis, Università di Siena, Siena, in preparation
Cited in the paper.
Defined as x ⋅ 1 − ( x / x 0 ) 2 ⋅ e − c A ⋅ ( x / x 0 ) 2 x\cdot\sqrt{1-(x/x_{0})^{2}}\cdot e^{-c_{\rm{A}}\cdot(x/x_{0})^{2}} if x < x 0 x<x_{0} , where x = m π + π − 2 x=m_{\pi^{+}\pi^{-}}^{2} . The cutoff x 0 x_{0} is extracted from the simulation while the coefficient c A c_{\rm A} is a free parameter in our fit. See H. Albrecht et al
Cited in the paper.