Predictions for $$\Xi _b^- \rightarrow \pi ^- (D_s^- ) \ \Xi _c^0 (2790) \left( \Xi _c^0 (2815) \right) $$ Ξ b - → π - ( D s - ) Ξ c 0 ( 2790 ) Ξ c 0 ( 2815 ) and $$\Xi _b^- \rightarrow \bar{\nu }_l l \ \Xi _c^0 (2790) \left( \Xi _c^0 (2815) \right) $$ Ξ b - → ν ¯ l l Ξ c 0 ( 2790 ) Ξ c 0 ( 2815 )

Abstract We have performed calculations for the nonleptonic $$\Xi _b^- \rightarrow \pi ^- \ \Xi _c^0 (2790) \left( J=\frac{1}{2}\right) $$ Ξ b - → π - Ξ c 0 ( 2790 ) J = 1 2 and $$\Xi _b^- \rightarrow \pi ^- \ \Xi _c^0 (2815) \left( J=\frac{3}{2}\right) $$ Ξ b - → π - Ξ c 0 ( 2815 ) J = 3 2 decays a...

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Bibliographic Details

Published in:	European Physical Journal C: Particles and Fields
Main Authors:	R. P. Pavao, Wei-Hong Liang, J. Nieves, E. Oset
Format:	Article
Language:	English
Published:	SpringerOpen 2017-04-01
Subjects:	Vector Meson Rest Frame Weak Decay Semileptonic Decay Radial Wave Function
Online Access:	http://link.springer.com/article/10.1140/epjc/s10052-017-4836-3