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Recent deviations from the standard model (SM) predictions of the experimental results on the R D ( * ) of the b → c l ν ̄ l semileptonic decay suggest the intervention of new physics (NP) mechanisms, which would affect the decay. Motivated by this, we investigate the possible NP effects on Ξ b → Ξ c τ ν ̄ τ and Ω b → Ω c τ ν ̄ τ processes in some NP models, such as the vector leptoquark (LQ) model, W′ model, aligned two-Higgs-doublet model and supersymmetry without R-parity model. Using the NP coupling parameter values obtained from different observables, we calculate various observables, such as the differential decay rate d B / d q 2 , the forward–backward asymmetry A FB l ( q 2 ) , the polarization fraction of final-state lepton and daughter baryon P L l ( q 2 ) as well as P L Ξ c ( Ω c ) ( q 2 ) , and the convexity parameter C F l ( q 2 ) in the SM and NP models. It is found that the SM predictions are consistent with those of previous works. In addition, the differential decay rate d B / d q 2 is quite sensitive to the contributions of some NP models. NP predictions generally show large deviations from the corresponding SM predictions. Nevertheless, the NP effects on some observables in the W′ model and LQ model are not sensitive, and these observables show the same variation tendency in the two NP models as in the SM.
Recent deviations from the standard model (SM) predictions of the experimental results on the R D ( * ) of the b → c l ν ̄ l semileptonic decay suggest the intervention of new physics (NP) mechanisms, which would affect the decay. Motivated by this, we investigate the possible NP effects on Ξ b → Ξ c τ ν ̄ τ and Ω b → Ω c τ ν ̄ τ processes in some NP models, such as the vector leptoquark (LQ) model, W′ model, aligned two-Higgs-doublet model and supersymmetry without R-parity model. Using the NP coupling parameter values obtained from different observables, we calculate various observables, such as the differential decay rate d B / d q 2 , the forward–backward asymmetry A FB l ( q 2 ) , the polarization fraction of final-state lepton and daughter baryon P L l ( q 2 ) as well as P L Ξ c ( Ω c ) ( q 2 ) , and the convexity parameter C F l ( q 2 ) in the SM and NP models. It is found that the SM predictions are consistent with those of previous works. In addition, the differential decay rate d B / d q 2 is quite sensitive to the contributions of some NP models. NP predictions generally show large deviations from the corresponding SM predictions. Nevertheless, the NP effects on some observables in the W′ model and LQ model are not sensitive, and these observables show the same variation tendency in the two NP models as in the SM.
In recent years, the experimental results about the ratio of the branching ratios $$R_{D^{(*)}}$$ R D ( ∗ ) and $$R_{K^{(*)}}$$ R K ( ∗ ) , which are in the semileptonic $$b\rightarrow c l \bar{\nu }_{l}$$ b → c l ν ¯ l and $$b\rightarrow s l^+l^-$$ b → s l + l - decays, have been observed to deviate from the Standard Model prediction by $$1.4\sigma $$ 1.4 σ , $$2.5\sigma $$ 2.5 σ , $$2.4\sigma $$ 2.4 σ and $$2.2\sigma $$ 2.2 σ respectively. Motivated by these anomalies and by the abundant $$B^*$$ B ∗ data samples, we investigate possible New Physics effects of the vector leptoquark in the semileptonic decay $$\bar{B}^*_{u,d,s,c} \rightarrow V \tau ^-\bar{\nu }_{\tau }$$ B ¯ u , d , s , c ∗ → V τ - ν ¯ τ ($$V=D^*_{u,d,s},J/\psi $$ V = D u , d , s ∗ , J / ψ ). which is induced by $$b\rightarrow c \tau ^-\bar{\nu }_{\tau }$$ b → c τ - ν ¯ τ at the quark level. Using the best fit solutions for the new operator Wilson coefficients and the relevant form factors which are obtained in the light-front quark model, we find that (i) the contributions of the vector leptoquark to $$d{\varGamma }^{(L)}/dq^2(\bar{B}^*_{u,d,s,c} \rightarrow V \tau ^-\bar{\nu }_{\tau })$$ d Γ ( L ) / d q 2 ( B ¯ u , d , s , c ∗ → V τ - ν ¯ τ ) and $$R^{*(L)}_{V}(q^2)$$ R V ∗ ( L ) ( q 2 ) to be significant; (ii) the two best fit solutions in the vector leptoquark are indistinguishable from each other and give similar amounts of enhancements to these two observables; (iii) both two cases of the vector leptoquark give nearly same results as those of the Standard Model for $$A_{FB}^{\tau }(q^2)$$ A FB τ ( q 2 ) , $$P_{\tau }(q^2)$$ P τ ( q 2 ) and $$F_{L}^{*V}(q^2)$$ F L ∗ V ( q 2 ) . We hope that the numerical results in this work will be tested in the future high energy experiments.
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