NLO twist-3 contributions to B → π form factors in kT factorization

被引:37
作者
Cheng, Shan [1 ,2 ]
Fan, Ying-Ying [1 ,2 ]
Yu, Xin [3 ,4 ]
Lu, Cai-Dian [3 ,4 ]
Xiao, Zhen-Jun [1 ,2 ,5 ]
机构
[1] Nanjing Normal Univ, Dept Phys, Nanjing 210023, Jiangsu, Peoples R China
[2] Nanjing Normal Univ, Inst Theoret Phys, Nanjing 210023, Jiangsu, Peoples R China
[3] Chinese Acad Sci, Inst High Energy Phys, Beijing 100049, Peoples R China
[4] Chinese Acad Sci, Theoret Phys Ctr Sci Facil, Beijing 100049, Peoples R China
[5] Nanjing Normal Univ, Jiangsu Key Lab Numer Simulat Large Scale Complex, Nanjing 210023, Jiangsu, Peoples R China
来源
PHYSICAL REVIEW D | 2014年 / 89卷 / 09期
基金
中国国家自然科学基金;
关键词
PERTURBATIVE QCD; WAVE-FUNCTIONS;
D O I
10.1103/PhysRevD.89.094004
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
In this paper, we calculate the next-to-leading-order (NLO) twist-3 contribution to the form factors of B -> pi transitions by employing the k(T) factorization theorem. All the infrared divergences regulated by the logarithms ln(k(iT)(2)) cancel between those from the quark diagrams and from the effective diagrams for the initial B meson wave function and the final pion meson wave function. An infrared finite NLO hard kernel is, therefore, obtained, which confirms the application of the k(T) factorization theorem to the B meson semileptonic decays at the twist-3 level. From our analytical and numerical evaluations, we find that the NLO twist-3 contributions to the form factors integral(+,0)(q(2)) of the B -> pi transition are similar in size but have an opposite sign with the NLO twist-2 contribution, which leads to a large cancellation between these two NLO parts. For the case of integral(+)(0), for example, the 24% NLO twist-2 enhancement to the full LO prediction is largely canceled by the negative (about -17%) NLO twist-3 contribution, leaving a small and stable 7% enhancement to the full LO prediction in the whole range of 0 <= q(2) <= 12 GeV2. At the full NLO level, the perturbative QCD prediction is F-B ->pi (0) = 0.269(-0.050)(+0.054).We also study the possible effects on the perturbative QCD predictions when different sets of the B meson and pion distribution amplitudes are used in the numerical evaluation.
引用
收藏
页数:18
相关论文
共 44 条
  • [1] [Anonymous], 1993, An Introduction to Quantum Field Theory
  • [2] Theoretical update of pseudoscalar meson distribution amplitudes of higher twist: the nonsinglet case
    Ball, P
    [J]. JOURNAL OF HIGH ENERGY PHYSICS, 1999, (01): : XX - 19
  • [3] Ball P, 1998, J HIGH ENERGY PHYS
  • [4] New results on B→π,K,η decay form factors from light-cone sum rules -: art. no. 014015
    Ball, P
    Zwicky, R
    [J]. PHYSICAL REVIEW D, 2005, 71 (01): : 014015 - 1
  • [5] Modelling light-cone distribution amplitudes from non-relativistic bound states
    Bell, G.
    Feldmann, Th.
    [J]. JOURNAL OF HIGH ENERGY PHYSICS, 2008, (04):
  • [6] QCD factorization for exclusive non-leptonic B-meson decays:: general arguments and the case of heavy-light final states
    Beneke, M
    Buchalla, G
    Neubert, M
    Sachrajda, CT
    [J]. NUCLEAR PHYSICS B, 2000, 591 (1-2) : 313 - 418
  • [7] Factorization of heavy-to-light form factors in soft-collinear effective theory
    Beneke, M
    Feldmann, T
    [J]. NUCLEAR PHYSICS B, 2004, 685 : 249 - 296
  • [8] HARD ELASTIC-SCATTERING IN QCD - LEADING BEHAVIOR
    BOTTS, J
    STERMAN, G
    [J]. NUCLEAR PHYSICS B, 1989, 325 (01) : 62 - 100
  • [9] B-meson distribution amplitude in QCD -: art. no. 034014
    Braun, VM
    Ivanov, DY
    Korchemsky, GP
    [J]. PHYSICAL REVIEW D, 2004, 69 (03):
  • [10] CONFORMAL-INVARIANCE AND PION WAVE-FUNCTIONS OF NONLEADING TWIST
    BRAUN, VM
    FILYANOV, IB
    [J]. ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS, 1990, 48 (02): : 239 - 247