Pure annihilation type decays B 0 →D − s K *+ 2 and B s →D̄a 2 in the perturbative QCD approach
Author:
Publisher
IOP Publishing
Subject
Astronomy and Astrophysics,Instrumentation,Nuclear and High Energy Physics
Reference29 articles.
1. B→M1M2: Factorization, charming penguins, strong phases, and polarization
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3. Direct CP violation in hadronic B decays
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5. B(Bs)→D(s)P,D(s)V,D(s)*P, andD(s)*Vdecays in the perturbative QCD approach
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1. Resonant contributions to three-body $$B\rightarrow KKK$$ decays in perturbative QCD approach;The European Physical Journal C;2020-05
2. Calculation of the $$B\rightarrow K_{0,2}^*(1430)f_0(980)/\sigma $$ decays in the perturbative QCD approach;The European Physical Journal C;2019-11
3. Quasi-two-body decays $$B \rightarrow D K^*(892) \rightarrow D K \pi $$ in the perturbative QCD approach;The European Physical Journal C;2019-06
4. The quasi-two-body decaysB(s)→(D(s),D¯(s))ρ→(D(s),D¯(s))ππin the perturbative QCD factorization approach;Nuclear Physics B;2017-10
5. Nonleptonic charmless decays of Bc→TP,TV in the perturbative QCD approach;Physical Review D;2017-07-20
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