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B K ? ν ν ˉ $$ Bo {K}^{left(st ight)}u overline{u} $$ decays in the Standard Model and beyond

机译: b k < / mi> ν ν ˉ $$ b to {k} ^ {左( AST 右)} nu overline { nu} $$ 标准型号及以后的衰减

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A bstract We present an analysis of the rare exclusive B decays B → K ν ν ˉ $$ Bo Ku overline{u} $$ and B → K ? ν ν ˉ $$ Bo {K}^{st}u overline{u} $$ within the Standard Model (SM), in a model-independent manner, and in a number of new physics (NP) models. Combining new form factor determinations from lattice QCD with light-cone sum rule results and including complete two-loop electroweak corrections to the SM Wilson coefficient, we obtain the SM predictions B R B + → K + ν ν ˉ = 4.0 ± 0.5 × 1 0 ? 6 $$ mathrm{B}mathrm{R}left({B}^{+}o {K}^{+}u overline{u}ight)=left(4.0pm 0.5ight)imes 1{0}^{-6} $$ and B R B 0 → K ? 0 ν ν ˉ = 9.2 ± 1.0 × 1 0 ? 6 $$ mathrm{B}mathrm{R}left({B}^0o {K}^{st 0}u overline{u}ight)=left(9.2pm 1.0ight)imes 1{0}^{-6} $$ , more precise and more robust than previous estimates. Beyond the SM, we make use of an effective theory with dimension-six operators invariant under the SM gauge symmetries to relate NP effects in b → s ν ν ˉ $$ bo su overline{u} $$ transitions to b → s? _(+) ? _(?)transitions and use the wealth of experimental data on B → K _((?)) ? _(+) ? _(?)and related modes to constrain NP effects in B → K ? ν ν ˉ $$ Bo {K}^{left(st ight)}u overline{u} $$ . We then consider several specific NP models, including Z ′ models, the MSSM, models with partial compositeness, and leptoquark models, demonstrating that the correlations between b → s ν ν ˉ $$ bo su overline{u} $$ observables among themselves and with B ~( s )?→? μ _(+) μ _(?)and b ?→? s? _(+) ? _(?)transitions offer powerful tests of NP with new right-handed couplings and non-MFV interactions.
机译:Bstract我们呈现了对罕见的独家B衰减B→kννν$$ b to k nu overline { nu} $$和b→k?在标准型号(SM)中,以型号独立的方式,以及许多新物理(NP)中的标准型号(SM)内ννˉ {k} nu overline { nu} $$ ) 楷模。将新的形式因子测定与光锥和规则结果的格子QCD相结合,包括完整的双环Electweak校正到SM Wilson系数,获得SM预测B R B +→K +νν= 4.0±0.5×1 0? 6 $$ mathrm {b} mathrm {r} left({b} ^ {+} to {k} ^ {+} nu overline { nu} rectle)= left(4.0 pm 0.5 右) times 1 {0} ^ { - 6} $$和brb 0→k? 0ννν= 9.2±1.0×1 0? 6 $$ mathrm {b} mathrm {r} left({b} ^ 0 to {k} ^ { ast 0} nu overline { nu} rectle)= left(9.2 pm 1.0 右) times 1 {0} ^ { - 6} $$,比以前的估计更精确,更强大。除了SM之外,我们利用了一个有效的理论,在SM仪表对称下的尺寸-6运算符不变,以在B→Sνν$$ b to s nu overline { nu} $$转换中涉及NP效果到b→s? _(+)? _(?)过渡并使用B→K _((?))的大量实验数据? _(+)? _(?)和相关模式来限制B→K中的NP效果? ννν$$ b to {k} ^ { left( ast 右)} nu overline { nu} $$。然后,我们考虑几个特定的​​NP模型,包括Z'模型,MSSM,具有部分合成度的模型和leptoquark模型,表明B→Sννˉˉ$$ b to s nu overline { nu}之间的相关性。 $$自己和b〜(s)之间的观察品?→? μ_(+)μ_(?)和b?→? s? _(+)? _(?)转换提供了具有新的右下耦合和非MFV交互的NP强大的测试。

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