English

On the Scale Uncertainties in the $B \to X_s \gamma$ Decay

High Energy Physics - Phenomenology 2009-10-30 v3

Abstract

We analyze the theoretical uncertainties in Br(BXsγ)Br(B\to X_s\gamma) due to the choice of the high energy matching scale μW=\ord(\mw)\mu_W=\ord(\mw) and the scale μt\mu_t at which the running top quark mass is defined: \mtb(μt)\mtb(\mu_t). To this end we have repeated the calculation of the initial conditions confirming the final results of Adel and Yao and Greub and Hurth and generalizing them to include the dependences on μt\mu_t and μW\mu_W with μtμW\mu_t\not=\mu_W. In the leading order the μW\mu_W and μt\mu_t uncertainties in Br(BXsγ)Br(B\to X_s\gamma) turn out to be ±13\pm 13% and ±3\pm 3% respectively. We show analytically how these uncertainties are reduced after including next-to-leading QCD corrections. They amount to ±1.1\pm 1.1% and ±0.4\pm 0.4% respectively. Reanalyzing the uncertainties due to the scale μb=\ord(mb)\mu_b=\ord(m_b) we find that after the inclusion of NLO effects they amount to ±4.3\pm 4.3% which is a factor 2/3 smaller than claimed in the literature. Including the uncertainties due to input parameters as well as the non-perturbative 1/mb21/m_b^2 and 1/mc21/m_c^2 corrections we find Br(BXsγ)=(3.60±0.33)×104Br(B{\to}X_s \gamma) = (3.60 \pm 0.33) \times 10^{-4} where the error is dominated by uncertainties in the input parameters. This should be compared with (3.28±0.33)×104(3.28 \pm 0.33) \times 10^{-4} found by Chetyrkin et al. where the error is shared evenly between the scale and parametric uncertainties.

Keywords

Cite

@article{arxiv.hep-ph/9707482,
  title  = {On the Scale Uncertainties in the $B \to X_s \gamma$ Decay},
  author = {Andrzej J. Buras and Axel Kwiatkowski and Nicolas Pott},
  journal= {arXiv preprint arXiv:hep-ph/9707482},
  year   = {2009}
}

Comments

11 pages, Latex. The paper is updated by incorporating recently modified results of the literature that were used for the numerical evaluation of eq. (17). A term originally missing in eq. (22) is added