Fetching the paper…
Reading the bibliography…
We report results from a search for the lepton flavor violating decays $B^0_{(s)}\to e^+\mu^-$, and the flavor-changing neutral-current decays $B^0_{(s)} \to e^+ e^-$.
J.C. Pati and A. Salam, Phys. Rev. D 10
1974
Earlier work this paper cites.
W. J. Marciano, Phys. Rev. D 29
1984
Earlier work this paper cites.
G. Valencia and S. Willenbrock, Phys. Rev. D 50
1994
Earlier work this paper cites.
F. Abe et al
1998
Earlier work this paper cites.
F. Abe et al
1998
Earlier work this paper cites.
M. Misiak and J. Urban, Phys. Lett. B 451
1999
Earlier work this paper cites.
A. Ilakovac, Phys. Rev. D 62
2000
Earlier work this paper cites.
2000
Cited alongside, same era.
E.J. Thomson et al
2002
Cited alongside, same era.
M. C. Chang et al
2003
Cited alongside, same era.
W. Ashmanskas et al
2004
Cited alongside, same era.
J. Bordes et al
2004
Cited alongside, same era.
R. A. Diaz, R. Martinez, C. E. Sandoval, Eur. Phys. J. C 41
2005
Cited alongside, same era.
D. Acosta et al
2005
Cited alongside, same era.
A. Abulencia et al
2006
Later among the works it cites.
A. Abulencia et al
2006
Later among the works it cites.
M. Blanke et al
2007
Later among the works it cites.
B. Aubert et al
2007
Later among the works it cites.
T. Aaltonen et al
2008
Later among the works it cites.
C. Amsler et al., Physics Letters B667, 1 (2008)
2008
Later among the works it cites.
alphaXiv searches the wider corpus for related work and actual follow-ups.
alphaXiv is searching for related work…
Throughout this Letter inclusion of charge conjugate reactions is implied
Cited in the paper.
The polar angle ( θ ) (\theta) in cylindrical coordinates is measured with respect to the proton beam direction, which defines the z z -axis. Pseudorapidity ( η ) (\eta) is defined as η = − ln ( tan θ 2 ) \eta=-\ln(\tan\frac{\theta}{2})
Cited in the paper.
The impact parameter d 0 d_{0} is the distance of closest approach of the track to the beam line
Cited in the paper.
Due to the hard b b -quark fragmentation, B B -mesons carry most of the momentum of the b b -quark. The isolation is defined as I = p T ( B ) / ( ∑ i p T i + p T ( B ) ) \mathit{I}=p_{T}(B)/(\sum_{i}p^{i}_{T}+p_{T}(B)) , 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 − ϕ \eta-\phi space around the B B flight direction
Cited in the paper.
For track pairs coming from the two-body decay of a B B , the vector pointing from the primary vertex to the B B decay vertex in the transverse plane l → x y \vec{l}_{xy} should point in the same direction as the transverse momentum vector p → T \vec{p}_{\rm{T}} (B) of the B B candidate. Δ ϕ \Delta\phi is defined as the angle between l → x y \vec{l}_{xy} and p → T ( B ) \vec{p}_{\rm{T}}(B)
Cited in the paper.