Threshold resummation for nonleptonic B meson decays
arXiv:hep-ph/0211272 · doi:10.1016/S0370-2693(03)00049-2
Abstract
We investigate the double logarithmic corrections , x being a parton momentum fraction, in two-body nonleptonic B meson decays in collinear factorization theorem of perturbative QCD (PQCD). It is found that these corrections are universal for factorizable amplitudes, {\it i.e.}, at the leading power, and that their threshold resummation smears the end-point singularities from . The double logarithmic corrections, depending on the topologies of nonfactorizable amplitudes at the subleading power, are negligible due to the color-transparency argument and to the overlap of three meson distribution amplitudes. We show that the PQCD approach to two-body nonleptonic B meson decays respects the factorization assumption in the heavy-quark limit.
10 pages, 4 figures
References in corpus (1)
Cited by in corpus (71)
- Charmless non-leptonic B_s decays to PP, PV and VV final states in the pQCD approach
- Resolution to the B -> pi K puzzle
- Next-to-leading-order corrections to form factors in factorization
- Polarizations in B -> VV decays
- Transition Form Factors in the PQCD approach
- Nonfactorizable contributions to decays
- B to tensor meson form factors in the perturbative QCD approach
- Branching ratio and CP asymmetry of decays in the perturbative QCD approach
- Transition form factors of B decays into p-wave axial-vector mesons in the perturbative QCD approach
- Pion transition form factor in k_T factorization
- Improved Estimates of The Decays in Perturbative QCD Approach
- Next-to-leading-order correction to pion form factor in factorization
- Vector-pseudoscalar two-meson distribution amplitudes in three-body meson decays
- Gluonic contribution to form factors
- Next-to-leading-order corrections to exclusive processes in factorization
- The pure annihilation type B_c to M_2 M_3 decays in the perturbative QCD approach
- The NLO twist-3 contributions to form factors in factorization
- meson wave function in factorization
- Branching ratio and CP violation of decays in the perturbative QCD approach
- The decays in perturbative QCD approach
- Next-to-leading-order time-like pion form factors in factorization
- Nonleptonic two-body charmless B decays involving a tensor meson in the Perturbative QCD Approach
- Polarization, CP Asymmetry and Branching ratios in B \to K^* K^* with Perturbative QCD approach
- The NLO twist-3 contribution to the pion electromagnetic form factors in factorization
- Time-like pion electromagnetic form factors in factorization with the Next-to-leading-order twist-3 contribution
- The and decays in perturbative QCD approach
- Direct CP Violation in Hadronic B Decays
- B meson wave function from the decay
- Branching Ratio and CP Asymmetry of Decays in the Perturbative QCD Approach
- B_s \to ρ(ω) K^* with Perturbative QCD approach
- Three-body decays in perturbative QCD approach
- , and -wave resonance contributions to decays in the perturbative QCD approach
- Nonleptonic charmless decays of in the perturbative QCD approach
- Reinvestigating the decays by including the contributions from
- decays and effects of the next-to-leading order contribution
- Decays in the Perturbative QCD Approach
- Phenomenological studies on the decays
- Branching ratio and CP violation of decays in the perturbative QCD approach
- Weak phases from topological-amplitude parametrization
- Branching Ratios and CP Violations of B \to K_0^*(1430) K^* Decays in the pQCD Approach
- Effect of resonance for asymmetry of the decay process in perturbative QCD
- The transition form factors in the Perturbative QCD factorization approach
- Direct violation of three bodies decay process from the resonance effect
- Nonleptonic decays of in the perturbative QCD approach
- violation induced by the double resonance for pure annihilation decay process in Perturbative QCD
- The perturbative QCD predictions for the decay B^{0}_{s}\rightarrow SS(a_{0}(980),f_{0}(980),f_{0}(500))
- Disentangling weak and strong interactions in Dalitz-plot analyses
- Penguin-dominated and decays in the perturbative QCD approach
- Direct violation for in Perturbative QCD
- Branching ratios of decays in perturbative QCD approach
- Reinvestigating the decays by including the contributions from with the perturbative QCD approach
- Perturbative QCD analysis of neutral -meson decays into and
- decays with mixing in the perturbative QCD approach
- Studies on the decays in the perturbative QCD approach
- Investigating three-body decays to scalar mesons in perturbative QCD approach
- Study of , , decays with perturbative QCD approach
- Study of the quasi-two-body decays B^{0}_{s} \rightarrow ψ(3770)(ψ(3686))π^+π^- with perturbative QCD approach
- Perturbative QCD for B_s \to a_1(1260)(b_1(1235))P(V) Decays
- Charmless hadronic decays in the perturbative QCD approach
- Study the contributions of S, P, and D-wave resonances to the quasi-two-body decays in perturbative QCD approach
- Phenomenological studies on neutral -meson decays into and
- Revisiting the decays in the perturbative QCD approach
- Next-to-Leading-logarithm threshold resummation for exclusive meson decays
- Possibility of experimental study on nonleptonic weak decays
- B\to K_1π(K) decays in the perturbative QCD approach
- Study of the decays
- Study of B^{0}_{s} \rightarrow \ TT(a_{2}(1320),K^{*}_{2}(1430),f_{2}(1270),f^{'}_{2}(1525)) in the perturbative QCD approach
- Study of parity violating and strangeness changing weak decays
- Study of quasi-two-body B^{0}\rightarrow T(ππ, K\bar{K},πη) decays in perturbative QCD approach
- Analysis of decays in the perturbative QCD approach
- Branching fraction, asymmetry, and polarization in decays with the modified perturbative QCD approach