Fetching the paper…
Reading the bibliography…
We present a search for the rare decays B+ -> K+ nu nubar and B0 -> K0 nu nubar using 459 million BBbar pairs collected with the BaBar detector at the SLAC National Accelerator Laboratory.
B. Efron and R. Tibshirani, An Introduction to the Bootstrap , Chapman & Hall (1993)
1993
Earlier work this paper cites.
L. Breiman, Mach. Learn. 24
1996
Earlier work this paper cites.
G. Buchalla, G. Hiller and G. Isidori, Phys. Rev. D 63
2000
Earlier work this paper cites.
R. Barlow, Application of the Bootstrap Resampling Technique to Particle Physics Experiments , Preprint MAN-HEP-99-4, (2000), www.hep.manchester.ac.uk/preprints/archive.html
2000
Earlier work this paper cites.
B. Aubert et al
2002
Earlier work this paper cites.
R. Barlow, Computer Physics Communications 149
2002
Earlier work this paper cites.
S. Agostinelli et al
2003
Earlier work this paper cites.
C. Bird, P. Jackson, R. V. Kowalewski and M. Pospelov, Phys. Rev. Lett. 93
2004
Cited alongside, same era.
B. Aubert et al
2005
Cited alongside, same era.
I. Narsky, arXiv:physics/0507157 (2005)
2005
Cited alongside, same era.
P. Colangelo, F. De Fazio, R. Ferrandes and T. N. Pham, Phys. Rev. D 73
2006
Cited alongside, same era.
T. M. Aliev, A. S. Cornell and N. Gaur, JHEP 0707
2007
Cited alongside, same era.
K. F. Chen et al
2007
Cited alongside, same era.
All kinematic quantities in this paper are defined in the lab frame unless marked with an asterisk, in which case they are in the CMS
B. Aubert et al
2007
Later among the works it cites.
Y. Yamada, Phys. Rev. D 77
2008
Later among the works it cites.
C. Amsler et al
2008
Later among the works it cites.
D. McKeen, Phys. Rev. D 79
2009
Later among the works it cites.
W. Altmannshofer, A. J. Buras, D. M. Straub and M. Wick, JHEP 0904
2009
Later among the works it cites.
B. Aubert et al
2009
Later among the works it cites.
alphaXiv searches the wider corpus for related work and actual follow-ups.
alphaXiv is searching for related work…
Cited in the paper.
Equal branching fractions for Υ ( 4 S ) → B 0 B ¯ 0 \mathchar 28935\relax{(4S)}\rightarrow B^{0}{\kern-1.60004pt\kern 1.79993pt\overline{\kern-1.79993ptB}{}^{0}} and Υ ( 4 S ) → B + B − \mathchar 28935\relax{(4S)}\rightarrow B^{+}{\kern-1.60004ptB^{-}} are assumed in this paper
Cited in the paper.