Search for b--> u transitions in B- -> [K+pi-pi0]_D K-

ARGUS Collaboration, H. Albrecht et al

Original

1990

Earlier work this paper cites.

M. Gronau and D. Wyler, Phys. Lett. B265

1991

Earlier work this paper cites.

PEP-II Conceptual Design Report, SLAC-0418 (1993)

1993

Earlier work this paper cites.

D. Atwood, I. Dunietz, and A. Soni, Phys. Rev. Lett. 78

2001

Earlier work this paper cites.

K. Cranmer, Comput. Phys. Commun. 136

2001

Earlier work this paper cites.

BaBar Collaboration, B. Aubert et al

2002

Cited alongside, same era.

BaBar Collaboration, B. Aubert et al

2002

Cited alongside, same era.

BaBar Collaboration, B. Aubert et al

2003

Cited alongside, same era.

Y. Grossman, A. Soffer and J. Zupan, Phys. Rev. D72

2005

Cited alongside, same era.

Charge conjugation is implied throughout the paper. Also, we use the notation B − → [ h 1 + ​ h 2 − ​ π 0 ] D ​ h 3 − B^{-}\rightarrow[h_{1}^{+}h_{2}^{-}\pi^{0}]_{D}h_{3}^{-} (with h i = π h_{i}=\pi or K K ) for the decay chains B − → D ~ 0 ​ h 3 − B^{-}\rightarrow\tilde{D}^{0}h_{3}^{-} , where D ~ 0 \tilde{D}^{0} is either a D 0 D^{0} or a D ¯ 0 \kern 1.99997pt\overline{\kern-1.99997ptD}{}^{0} and D ~ 0 → h 1 + ​ h 2 − ​ π 0 \tilde{D}^{0}~\rightarrow h_{1}^{+}h_{2}^{-}\pi^{0} . We also refer to h 3 h_{3} as the π \pi or K K from the B B

Cited in the paper.

BaBar Collaboration, B. Aubert et al

2005

Later among the works it cites.

BaBar Collaboration, B. Aubert et al

2005

Later among the works it cites.

Particle Data Group, S. Eidelman et al

2005

Later among the works it cites.

BaBar Collaboration, B. Aubert et al

2006

Later among the works it cites.