On the Scale Uncertainties in the $B \to X_s \gamma$ Decay
Phys.Lett. B414 (1997) 157-165; Erratum-ibid. B434 (1998) 459 We analyze the theoretical uncertainties in $Br(B\to X_s\gamma)$ due to the choice of the high energy matching scale $\mu_W=\ord(\mw)$ and the scale $\mu_t$ at which the running top quark mass is defined: $\mtb(\mu_t)$. To this end we hav...
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Zusammenfassung: | Phys.Lett. B414 (1997) 157-165; Erratum-ibid. B434 (1998) 459 We analyze the theoretical uncertainties in $Br(B\to X_s\gamma)$ due to the
choice of the high energy matching scale $\mu_W=\ord(\mw)$ and the scale
$\mu_t$ at which the running top quark mass is defined: $\mtb(\mu_t)$. 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 $\mu_t$ and $\mu_W$ with $\mu_t\not=\mu_W$. In the
leading order the $\mu_W$ and $\mu_t$ uncertainties in $Br(B\to X_s\gamma)$
turn out to be $\pm 13%$ and $\pm 3%$ respectively. We show analytically how
these uncertainties are reduced after including next-to-leading QCD
corrections. They amount to $\pm 1.1%$ and $\pm 0.4%$ respectively. Reanalyzing
the uncertainties due to the scale $\mu_b=\ord(m_b)$ we find that after the
inclusion of NLO effects they amount to $\pm 4.3%$ 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 $1/m_b^2$ and $1/m_c^2$
corrections we find $Br(B{\to}X_s \gamma) = (3.60 \pm 0.33) \times 10^{-4}$
where the error is dominated by uncertainties in the input parameters. This
should be compared with $(3.28 \pm 0.33) \times 10^{-4}$ found by Chetyrkin et
al. where the error is shared evenly between the scale and parametric
uncertainties. |
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DOI: | 10.48550/arxiv.hep-ph/9707482 |