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Axel Kwiatkowski

Publications and source records attributed to Axel Kwiatkowski.

3 recordsLinked to original sources

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

We analyze the theoretical uncertainties in $Br(B\to X_sγ)$ due to the choice of the high energy matching scale $μ_W=\ord(\mw)$ and the scale $μ_t$ at which the running top quark mass is defined: $\mtb(μ_t)$. 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 $μ_t$ and $μ_W$ with $μ_t\not=μ_W$. In the leading order the $μ_W$ and $μ_t$ uncertainties in $Br(B\to X_sγ)$ 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 $μ_b=\ord(m_b)$ 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 $Br(B{\to}X_s γ) = (3.60 \pm 0.33) \times 10^{-4}$ 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.

hep-ph

Parton model sum rules

This review article discusses the experimental and theoretical status of various Parton Model sum rules. The basis of the sum rules in perturbative QCD is discussed. Their use in extracting the value of the strong coupling constant is evaluated and the failure of the naive version of some of these rules is assessed.

hep-ph

The $\msbar$ Renormalized Bottom Mass of Order ${\cal O}(α_s G_F M_t^2)$ and its Application to $Γ(H\to b\bar{b})$

The renormalized mass of the bottom quark is calculated at the two loop level to order ${\cal O}(α_s G_F M_t^2)$ in the $\msbar$ renormalization scheme. Different strategies for the computation are outlined. The result is applied to the partial decay rate $Γ(H\rightarrow b\bar{b})$ of the Higgs boson into bottom quarks. Expressing the width in terms of the running mass instead of the bottom pole mass allows to treat the ${\cal O}(α_s G_F M_t^2)$ radiative corrections on the same footing as is commonly used in pure QCD calculations. The numerical values for the corrections are given and the sizes of different contributions are compared.

hep-ph