Abstract <p>In the Belle experiment, the branching fractions for inclusive decays of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(B_{s}^{0}\)</EquationSource> <!--NuclPhys2560192Yasaveev-m5--> </InlineEquation> mesons into <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(D\)</EquationSource> <!--NuclPhys2560192Yasaveev-m6--> </InlineEquation> mesons are measured using the hadron tagging method. The results are obtained using a data sample with a total luminosity of 121.4 fb<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({}^{-1}\)</EquationSource> <!--NuclPhys2560192Yasaveev-m7--> </InlineEquation> collected at the energy of the <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\Upsilon(5S)\)</EquationSource> <!--NuclPhys2560192Yasaveev-m8--> </InlineEquation> resonance by the Belle detector at the KEKB asymmetric electron–positron collider. We obtain <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathcal{B}(B_{s}^{0}\to D_{s}^{\pm}X)=(68.6\pm 7.2\pm 4.0)\%\)</EquationSource> <!--NuclPhys2560192Yasaveev-m9--> </InlineEquation>, <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mathcal{B}(B_{s}^{0}\to D^{0}/\bar{D}^{0}X)=(21.5\pm 6.1\pm 1.8)\%\)</EquationSource> <!--NuclPhys2560192Yasaveev-m10--> </InlineEquation>, and <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\mathcal{B}(B_{s}^{0}\to D^{\pm}X)=(12.6\pm 4.6\pm 1.3)\%\)</EquationSource> <!--NuclPhys2560192Yasaveev-m11--> </InlineEquation>. The branching fractions for the inclusive decays into <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(D_{s}^{\pm}\)</EquationSource> <!--NuclPhys2560192Yasaveev-m12--> </InlineEquation> and <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(D^{0}/\bar{D}^{0}\)</EquationSource> <!--NuclPhys2560192Yasaveev-m13--> </InlineEquation> are consistent with previous Belle measurements. The new value of <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\mathcal{B}(B_{s}^{0}\to D_{s}^{\pm}X)\)</EquationSource> <!--NuclPhys2560192Yasaveev-m14--> </InlineEquation> allows us to obtain the energy dependence of <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(e^{+}e^{-}\to B_{s}^{0}\bar{B}_{s}^{0}X\)</EquationSource> <!--NuclPhys2560192Yasaveev-m15--> </InlineEquation> cross section and <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(B_{s}^{0}\)</EquationSource> <!--NuclPhys2560192Yasaveev-m16--> </InlineEquation> mesons’ production rate at the energy of the <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\Upsilon(5S)\)</EquationSource> <!--NuclPhys2560192Yasaveev-m17--> </InlineEquation> resonance, <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(f_{s}=(21.4^{+1.5}_{-1.4})\%\)</EquationSource> <!--NuclPhys2560192Yasaveev-m18--> </InlineEquation>, with more accuracy.</p>

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Measurement of \({\mathcal{B}(B_{s}^{0}\to D/\bar{D}X)}\) with \({B_{s}}\) Hadronic Tagging

  • M. Yasaveev

摘要

Abstract

In the Belle experiment, the branching fractions for inclusive decays of \(B_{s}^{0}\) mesons into \(D\) mesons are measured using the hadron tagging method. The results are obtained using a data sample with a total luminosity of 121.4 fb \({}^{-1}\) collected at the energy of the \(\Upsilon(5S)\) resonance by the Belle detector at the KEKB asymmetric electron–positron collider. We obtain \(\mathcal{B}(B_{s}^{0}\to D_{s}^{\pm}X)=(68.6\pm 7.2\pm 4.0)\%\) , \(\mathcal{B}(B_{s}^{0}\to D^{0}/\bar{D}^{0}X)=(21.5\pm 6.1\pm 1.8)\%\) , and \(\mathcal{B}(B_{s}^{0}\to D^{\pm}X)=(12.6\pm 4.6\pm 1.3)\%\) . The branching fractions for the inclusive decays into \(D_{s}^{\pm}\) and \(D^{0}/\bar{D}^{0}\) are consistent with previous Belle measurements. The new value of \(\mathcal{B}(B_{s}^{0}\to D_{s}^{\pm}X)\) allows us to obtain the energy dependence of \(e^{+}e^{-}\to B_{s}^{0}\bar{B}_{s}^{0}X\) cross section and \(B_{s}^{0}\) mesons’ production rate at the energy of the \(\Upsilon(5S)\) resonance, \(f_{s}=(21.4^{+1.5}_{-1.4})\%\) , with more accuracy.