Three-body decays 
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>B</mml:mi><mml:mo stretchy="false">→</mml:mo><mml:mi>ϕ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mi>ρ</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mi>K</mml:mi><mml:mi>γ</mml:mi></mml:mrow></mml:math>
 in perturbative QCD approach

Wang, Chao; Liu, Jing; Li, Hsiang-nan; Lü, C.

doi:10.1103/physrevd.97.034033

Cited by 26 publications

(31 citation statements)

References 103 publications

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“…Relying on the perturbative QCD (PQCD) approach, furthermore, some three-body B meson decays have also been investigated in Refs. [44][45][46][47]. The authors of Ref.…”

Section: Introductionmentioning

confidence: 99%

Quasi-two-body decays B(s)→Pf2(1270)<

Xiao

Wang

et al. 2018

Phys. Rev. D

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In this work, we calculate the CP-averaged branching ratios and direct CP-violating asymmetries of the quasi-two-body decays B ðsÞ → Pf 2 ð1270Þ → Pππ with the two-pion distribution amplitude Φ D ππ by using the perturbative QCD factorization approach, where P represents a light pseudoscalar meson K, π, η and η 0. The relativistic Breit-Wigner formula for the D-wave resonance f 2 ð1270Þ is adopted to parameterize the timelike form factor F π , which contains the final state interactions between the pions in the resonant regions. The consistency of theoretical results with data can be achieved by determining the Gegenbauer moments of the D-wave two-pion distribution amplitudes. The decay rates for the considered decay modes are generally in the order of 10 −9 to 10 −6. The integrated direct CP asymmetries for the charged modes agree with the BABAR and Belle measurements. As a by-product, we extract the branching ratios of B ðsÞ → Pf 2 ð1270Þ from the corresponding quasi-two-body decay modes, which still need experimental tests at the ongoing and forthcoming experiments.

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“…Relying on the perturbative QCD (PQCD) approach, furthermore, some three-body B meson decays have also been investigated in Refs. [44][45][46][47]. The authors of Ref.…”

Section: Introductionmentioning

confidence: 99%

Quasi-two-body decays B(s)→Pf2(1270)<

Xiao

Wang

et al. 2018

Phys. Rev. D

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“…The perturbative QCD (PQCD) factorization approach has been employed in Refs. [34][35][36][37][38], where the strong dynamics between the two final state hadrons in resonant regions are factorized into a new non-perturbative input, the twohadron distribution amplitudes (DAs) h 1 h 2 [39][40][41][42][43][44][45]. Both nonresonant and resonant contributions can be accommodated into this new input in PQCD factorization approach.…”

Section: Introductionmentioning

confidence: 99%

Quasi-two-body decays $$B_{(s)}\rightarrow K^*(892)h\rightarrow K\pi h$$ B ( s ) → K ∗ ( 892 ) h → K π h in perturbative QCD approach

et al. 2019

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We extend our recent works on the P-wave twopion resonant contributions to the kaon-pion cases in the hadronic charmless B meson decays by employing the perturbative QCD approach. The concerned decay modes are analysed in the quasi-two-body framework by parameterizing the kaon-pion distribution amplitude P K π , which contains the final state interactions between the kaon and pion in the resonant region. The relativistic Breit-Wigner formula for the Pwave resonant state K * (892) is adopted to parameterize the time-like form factor F K π. We calculate the C P-averaged branching ratios and direct C P-violating asymmetries of the quasi-two-body decays B (s) → K * (892)h → K π h, with h = (π, K), in this work. It is shown that the agreement of theoretical results with the experimental data can be achieved, through which Gegenbauer moments of the Pwave kaon-pion distribution amplitudes are determined. The predictions in this work will be tested by the precise data from the LHCb and the future Belle II experiments.

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“…In recent years, within PQCD approach, the quasi-twobody B meson decays including ππ pair and K π pair through the S, P, and D wave resonances have been studied extensively [49][50][51][52][53][54][55][56][57][58][59][60][61]. In ref.…”

Section: Introductionmentioning

confidence: 99%

Resonant contributions to three-body $$B\rightarrow KKK$$ decays in perturbative QCD approach

Liu

2020

Eur. Phys. J. C

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In this work, we study the (S, P and D)-wave K + K − contributions to B → K K K decays in the perturbative QCD approach at leading order. Within the two-meson wave functions describing the nonperturbative dynamics in the kaon-pair for different waves, we calculate the branching fractions and the direct C P asymmetries of these decay modes in the corresponding resonance regions. Most of our numerical results are well consistent with the current measurements. We note that the narrow-width approximation is invalid in the quasi-two-body decays B → K f 0 (980) → K K K. For other decays, under the narrow-width approximation we can extract the branching fractions of the corresponding two-body decays involving the intermediate resonant states, and the related branching fractions agree with the current experimental data well. Furthermore, we also predict the branching fractions of the corresponding quasi-two-body decays B → K π + π − , which are expected to be tested in the ongoing LHCb and Belle-II experiments.

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Three-body decays B→ϕ(ρ)Kγ in perturbative QCD approach

Cited by 26 publications

References 103 publications

Quasi-two-body decays B(s)→Pf2(1270)<

Quasi-two-body decays B(s)→Pf2(1270)<

Quasi-two-body decays $$B_{(s)}\rightarrow K^*(892)h\rightarrow K\pi h$$ B ( s ) → K ∗ ( 892 ) h → K π h in perturbative QCD approach

Resonant contributions to three-body $$B\rightarrow KKK$$ decays in perturbative QCD approach

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