<p>This study focuses on the decay of the <i>B</i><sub><i>c</i></sub> meson to S-wave charmonia. Starting with lattice inputs on <i>B</i><sub><i>c</i></sub> → <i>J</i>/<i>ψ</i> form factors, we have obtained the <i>B</i><sub><i>c</i></sub> → <i>η</i><sub><i>c</i></sub> form factors using heavy quark spin symmetry (HQSS) relations between the associated form factors after parametrizing and extracting the possible symmetry breaking corrections. Using the <i>q</i><sup>2</sup> shapes of these form factors, we have computed the branching fractions <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">B</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{B} \)</EquationSource> </InlineEquation>(<InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>B</mi> <mi>c</mi> <mo>−</mo> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {B}_c^{-} \)</EquationSource> </InlineEquation> → <i>η</i><sub><i>c</i></sub><i>ℓ</i><sup><i>−</i></sup><InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math display="inline"> <mover accent="true"> <mi>ν</mi> <mo stretchy="true">¯</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">\( \overline{\nu} \)</EquationSource> </InlineEquation>) (with <i>ℓ</i> = <i>τ, μ</i>(<i>e</i>)) and the decay rate distributions and have predicted the Standard model estimate for the observable <i>R</i>(<i>η</i><sub><i>c</i></sub>) = Γ(<InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>B</mi> <mi>c</mi> <mo>−</mo> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {B}_c^{-} \)</EquationSource> </InlineEquation> → <i>η</i><sub><i>c</i></sub><i>τ</i><sup><i>−</i></sup><InlineEquation ID="IEq5"> <EquationSource Format="MATHML"><math display="inline"> <mover accent="true"> <mi>ν</mi> <mo stretchy="true">¯</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">\( \overline{\nu} \)</EquationSource> </InlineEquation>)/Γ(<InlineEquation ID="IEq6"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>B</mi> <mi>c</mi> <mo>−</mo> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {B}_c^{-} \)</EquationSource> </InlineEquation> <i>→ η</i><sub><i>c</i></sub><i>μ</i><sup><i>−</i></sup><InlineEquation ID="IEq7"> <EquationSource Format="MATHML"><math display="inline"> <mover accent="true"> <mi>ν</mi> <mo stretchy="true">¯</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">\( \overline{\nu} \)</EquationSource> </InlineEquation>) = 0<i>.</i>310 <i>±</i> 0<i>.</i>042. In addition, we have estimated the radial wave functions <InlineEquation ID="IEq8"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>ψ</mi> <msub> <mi>B</mi> <mi>c</mi> </msub> <mi>R</mi> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {\psi}_{B_c}^R \)</EquationSource> </InlineEquation> (0), <InlineEquation ID="IEq9"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>ψ</mi> <mrow> <mi>J</mi> <mo>/</mo> <mi>ψ</mi> </mrow> <mi>R</mi> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {\psi}_{J/\psi}^R \)</EquationSource> </InlineEquation> (0) and <InlineEquation ID="IEq10"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>ψ</mi> <msub> <mi>η</mi> <mi>c</mi> </msub> <mi>R</mi> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {\psi}_{\eta_c}^R \)</EquationSource> </InlineEquation> (0) at small <i>Bc J</i>/<i>ψ ηc</i> quark-antiquark distances from the available information on the form factors from lattice, the lattice inputs on the decay constants <i>f</i><sub><i>J</i>/<i>ψ</i></sub>, <InlineEquation ID="IEq11"> <EquationSource Format="MATHML"><math display="inline"> <msub> <mi>f</mi> <msub> <mi>η</mi> <mi>c</mi> </msub> </msub> </math></EquationSource> <EquationSource Format="TEX">\( {f}_{\eta_c} \)</EquationSource> </InlineEquation>, <InlineEquation ID="IEq12"> <EquationSource Format="MATHML"><math display="inline"> <msub> <mi>f</mi> <msub> <mi>B</mi> <mi>c</mi> </msub> </msub> </math></EquationSource> <EquationSource Format="TEX">\( {f}_{B_c} \)</EquationSource> </InlineEquation> and experimental data on radiative and rare decays of the <i>J</i>/<i>ψ</i> and <i>η</i><sub><i>c</i></sub> mesons. To do so, we choose the theory framework of non-relativistic QCD (NRQCD) effective theory. Using our results, we have predicted the branching fractions of a few non-leptonic decays of <i>B</i><sub><i>c</i></sub> → <i>J</i>/<i>ψ</i> or <i>η</i><sub><i>c</i></sub> and other light mesons. We have also updated the numerical estimates of the cross sections <i>σ</i>(<i>e</i><sup>+</sup><i>e</i><sup><i>−</i></sup> → <i>J</i>/<i>ψη</i><sub><i>c</i></sub><i>, η</i><sub><i>c</i></sub><i>γ</i>) and predicted the branching fractions of <i>Z</i> boson decays to either <i>J</i>/<i>ψ</i> or <i>η</i><sub><i>c</i></sub> final states or both.</p>

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Analyzing the semileptonic and nonleptonic BcJ/ψ, ηc decays

  • Aritra Biswas,
  • Soumitra Nandi,
  • Shantanu Sahoo

摘要

This study focuses on the decay of the Bc meson to S-wave charmonia. Starting with lattice inputs on BcJ/ψ form factors, we have obtained the Bcηc form factors using heavy quark spin symmetry (HQSS) relations between the associated form factors after parametrizing and extracting the possible symmetry breaking corrections. Using the q2 shapes of these form factors, we have computed the branching fractions B \( \mathcal{B} \) ( B c \( {B}_c^{-} \) ηc ν ¯ \( \overline{\nu} \) ) (with = τ, μ(e)) and the decay rate distributions and have predicted the Standard model estimate for the observable R(ηc) = Γ( B c \( {B}_c^{-} \) ηcτ ν ¯ \( \overline{\nu} \) )/Γ( B c \( {B}_c^{-} \) → ηcμ ν ¯ \( \overline{\nu} \) ) = 0.310 ± 0.042. In addition, we have estimated the radial wave functions ψ B c R \( {\psi}_{B_c}^R \) (0), ψ J / ψ R \( {\psi}_{J/\psi}^R \) (0) and ψ η c R \( {\psi}_{\eta_c}^R \) (0) at small Bc J/ψ ηc quark-antiquark distances from the available information on the form factors from lattice, the lattice inputs on the decay constants fJ/ψ, f η c \( {f}_{\eta_c} \) , f B c \( {f}_{B_c} \) and experimental data on radiative and rare decays of the J/ψ and ηc mesons. To do so, we choose the theory framework of non-relativistic QCD (NRQCD) effective theory. Using our results, we have predicted the branching fractions of a few non-leptonic decays of BcJ/ψ or ηc and other light mesons. We have also updated the numerical estimates of the cross sections σ(e+eJ/ψηc, ηcγ) and predicted the branching fractions of Z boson decays to either J/ψ or ηc final states or both.