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Theoretical update ofBs−bar Bsmixing
Author(s) -
Alexander Lenz,
Ulrich Nierste
Publication year - 2007
Publication title -
journal of high energy physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.998
H-Index - 261
eISSN - 1126-6708
pISSN - 1029-8479
DOI - 10.1088/1126-6708/2007/06/072
Subject(s) - physics , particle physics , hadron , observable , cp violation , asymmetry , cabibbo–kobayashi–maskawa matrix , mixing (physics) , matrix (chemical analysis) , quark , quantum mechanics , materials science , composite material
We update the theory predictions for the mass difference $\dm_s$, the widthdifference $\dg_s$ and the CP asymmetry in flavour-specific decays, $a_{\rmfs}^{s}$, for the \bbs system. In particular we present a new expression forthe element $\Gamma_{12}^s$ of the decay matrix, which enters the predictionsof $\dg_s$ and $a_{\rm fs}^{s}$. To this end we introduce a new operator basis,which reduces the troublesome sizes of the $1/m_b$ and $\alpha_s$ correctionsand diminishes the hadronic uncertainty in $\dg_s/\dm_s$ considerably.Logarithms of the charm quark mass are summed to all orders. We find$\dg_s/\dm_s= (49.7 \pm 9.4) \cdot 10^{-4}$ and $\dg_s =(f_{B_s}/240 {\rmMeV})^2 [(0.105 \pm 0.016) B + (0.024 \pm 0.004) \tilde{B}_S' - 0.027 \pm0.015] {ps}^{-1}$ in terms of the bag parameters $B$, $\tilde{B}_S'$ in the NDRscheme and the decay constant $f_{B_s}$. The improved result for$\Gamma_{12}^s$ also permits the extraction of the CP-violating \bbms phasefrom $a_{\rm fs}^{s}$ with better accuracy. We show how the measurements of$\Delta M_s$, $\Delta\Gamma_s$, $a_{\rm fs}^{s}$, $A_{\rm CP}^{\rm mix}(B_s\toJ/\psi \phi)$ and other observables can be efficiently combined to constrainnew physics. Applying our new formulae to data from the D{\O}experiment, wefind a 2$\sigma$ deviation of the \bbms phase from its Standard Model value. Wealso briefly update the theory predictions for the \bbd system and find$\dg_d/\dm_d = \lt(52.6 \epm{11.5}{12.8} \rt) \cdot 10^{-4}$ and $a_{\rm fs}^d= \lt(-4.8\epm{1.0}{1.2} \rt) \cdot 10^{-4}$ in the Standard Model.Comment: 38 pages, 7 figures, revised version to appear in JHEP, comments added. We correct the incorrect use of an experimental input in eq. (93) and Fig. 7. Our conclusions remain unchange

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