Genuine lepton-flavor-universality-violating observables in the $τ-μ$ sector of $B \to (K,\,K^*) \ell \ell $ decays

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Hauptverfasser: Alok, Ashutosh Kumar, Chundawat, Neetu Raj Singh, Kumar, Jitendra, Mandal, Arindam, Tamponi, Umberto
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Veröffentlicht: 2024
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author Alok, Ashutosh Kumar
Chundawat, Neetu Raj Singh
Kumar, Jitendra
Mandal, Arindam
Tamponi, Umberto
author_facet Alok, Ashutosh Kumar
Chundawat, Neetu Raj Singh
Kumar, Jitendra
Mandal, Arindam
Tamponi, Umberto
contents It was previously shown that unlike the ratios $R_K^{μe} \equiv R_K \equiv Γ(B \to K μ^+ μ^-)/Γ(B \to K e^+ e^-)$ and $R_{K^*}^{μe} \equiv R_{K^*} \equiv Γ(B \to K^* μ^+ μ^-)/Γ(B \to K^* e^+ e^-)$, the ratios $R_K^{τμ}$ and $R_{K^*}^{τμ}$ can deviate from their Standard Model (SM) predictions even with universal new physics couplings. This observation highlights the critical need to identify and establish genuine lepton flavor universality violating (LFUV) observables in the $τ-μ$ sector. This work embarks on establishing genuine LFUV ratio observables in $B \to K \ell \ell$ and $B \to K^* \ell \ell$ decays through comprehensive analysis of their angular distributions. We find that like $R_{K^*}^{τμ}$, the ratios $R_{A_{FB}}^{τμ}$ and $R_{f_L}^{τμ}$ do not qualify as genuine LFUV observables, whereas the ratios of all optimized observables in $B \to K^* \ell \ell$ decays within the $τ-μ$ sector definitively do. In the case of $B \to K \ell \ell$ decays, similar to $R_K^{τμ}$, the ratio $R_{F_H}$ is influenced by mass effects and therefore cannot be considered a genuine LFUV observable in the $τ-μ$ sector. However, the ratio $Γ_τ(1-F_{H}^τ)/Γ_μ(1-F_{H}^μ)$ stands as the sole genuine LFUV observable in $B \to K \ell \ell$ decays. Furthermore, by making use of new physics Lorentz structures which provide a better fit to the current $b \to s \ell \ell$ data as compared to the SM, we demonstrate how the non-genuine LFUV ratios $R_{A_{FB}}^{τμ}$ and $R_{f_L}^{τμ}$ can be employed to distinguish between framework with solely universal lepton couplings and those with both universal and non-universal couplings.
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publishDate 2024
record_format arxiv
spellingShingle Genuine lepton-flavor-universality-violating observables in the $τ-μ$ sector of $B \to (K,\,K^*) \ell \ell $ decays
Alok, Ashutosh Kumar
Chundawat, Neetu Raj Singh
Kumar, Jitendra
Mandal, Arindam
Tamponi, Umberto
High Energy Physics - Phenomenology
High Energy Physics - Experiment
It was previously shown that unlike the ratios $R_K^{μe} \equiv R_K \equiv Γ(B \to K μ^+ μ^-)/Γ(B \to K e^+ e^-)$ and $R_{K^*}^{μe} \equiv R_{K^*} \equiv Γ(B \to K^* μ^+ μ^-)/Γ(B \to K^* e^+ e^-)$, the ratios $R_K^{τμ}$ and $R_{K^*}^{τμ}$ can deviate from their Standard Model (SM) predictions even with universal new physics couplings. This observation highlights the critical need to identify and establish genuine lepton flavor universality violating (LFUV) observables in the $τ-μ$ sector. This work embarks on establishing genuine LFUV ratio observables in $B \to K \ell \ell$ and $B \to K^* \ell \ell$ decays through comprehensive analysis of their angular distributions. We find that like $R_{K^*}^{τμ}$, the ratios $R_{A_{FB}}^{τμ}$ and $R_{f_L}^{τμ}$ do not qualify as genuine LFUV observables, whereas the ratios of all optimized observables in $B \to K^* \ell \ell$ decays within the $τ-μ$ sector definitively do. In the case of $B \to K \ell \ell$ decays, similar to $R_K^{τμ}$, the ratio $R_{F_H}$ is influenced by mass effects and therefore cannot be considered a genuine LFUV observable in the $τ-μ$ sector. However, the ratio $Γ_τ(1-F_{H}^τ)/Γ_μ(1-F_{H}^μ)$ stands as the sole genuine LFUV observable in $B \to K \ell \ell$ decays. Furthermore, by making use of new physics Lorentz structures which provide a better fit to the current $b \to s \ell \ell$ data as compared to the SM, we demonstrate how the non-genuine LFUV ratios $R_{A_{FB}}^{τμ}$ and $R_{f_L}^{τμ}$ can be employed to distinguish between framework with solely universal lepton couplings and those with both universal and non-universal couplings.
title Genuine lepton-flavor-universality-violating observables in the $τ-μ$ sector of $B \to (K,\,K^*) \ell \ell $ decays
topic High Energy Physics - Phenomenology
High Energy Physics - Experiment
url https://arxiv.org/abs/2405.18488