Electromagnetic dipole operator effect on (B)over bar→Xsγ at partial derivative(αs2) -: art. no. 033014

被引:56
作者
Blokland, I [1 ]
Czarnecki, A
Misiak, M
Slusarczyk, M
Tkachov, F
机构
[1] Univ Alberta, Dept Phys, Edmonton, AB T6G 2J1, Canada
[2] Univ Victoria, Dept Phys & Astron, Victoria, BC V8P 5C2, Canada
[3] Univ Warsaw, Inst Theoret Phys, PL-00681 Warsaw, Poland
[4] Jagiellonian Univ, Inst Phys, PL-30059 Krakow, Poland
[5] Russian Acad Sci, Inst Nucl Res, Moscow 117312, Russia
来源
PHYSICAL REVIEW D | 2005年 / 72卷 / 03期
关键词
D O I
10.1103/PhysRevD.72.033014
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The flavor-changing electromagnetic dipole operator O-7 gives the dominant contribution to the (B) over bar -> X(s)gamma decay rate. We calculate two-loop QCD corrections to its matrix element together with the corresponding bremsstrahlung contributions. The optical theorem is applied, and the relevant imaginary parts of three-loop diagrams are computed following the lines of our recent t -> XbW calculation. The complete result allows us to test the validity of the naive non-Abelianization (NNA) approximation that has been previously applied to estimate the next-to-next-to-leading order QCD correction to Gamma(<(B)overbar >-> X(s)gamma)/Gamma((B) over bar -> X(u)e <(nu)over bar >). When both decay widths are normalized to m(b,R)(5) in the same renormalization scheme R, the calculated O(alpha(s)(2)) correction is sizable (similar to 6%), and the NNA estimate is about 1/3 too large. On the other hand, when the ratio of the decay widths is written as Sxm(b)(<(MS)over bar >)(2)(m(b))/m(b,pole)(2), the calculated O(alpha(s)(2)) correction to S is at the level of 1% for both the complete and the NNA results.
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页码:1 / 8
页数:8
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