Covariant light-front calculations predict branching ratios of 10^{-5} to 10^{-3} for B(s) to D(s)(2S) and D*(s)(2S) plus light mesons, larger than Bethe-Salpeter results but consistent with other quark models.
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Perturbative QCD calculations yield branching fractions 10^{-9} to 10^{-4} for B to P D0*(2400) to P D pi decays plus several ratios consistent with SU(3) symmetry.
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$D_{(s)}(2S)$ and $D^{*}_{(s)}(2S)$ production in nonleptonic $B_{(s)}$ weak decays
Covariant light-front calculations predict branching ratios of 10^{-5} to 10^{-3} for B(s) to D(s)(2S) and D*(s)(2S) plus light mesons, larger than Bethe-Salpeter results but consistent with other quark models.
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Quasi-two-body decays $B_{(s)} \to P D_0^*(2400) \to P D \pi$ in the perturbative QCD approach
Perturbative QCD calculations yield branching fractions 10^{-9} to 10^{-4} for B to P D0*(2400) to P D pi decays plus several ratios consistent with SU(3) symmetry.