On the contribution of the electromagnetic dipole operator O7{\cal O}_7 to the Bˉs→μ+μ−\bar B_s \to \mu^+\mu^- decay amplitude

We construct a factorization theorem that allows to systematically include QCD corrections to the contribution of the electromagnetic dipole operator in the effective weak Hamiltonian to the $\bar B_s \to \mu^+\mu^-$ decay amplitude. We first rederive the known result for the leading-order QED box diagram, which features a double-logarithmic enhancement associated to the different rapidities of the light quark in the $\bar B_s$ meson and the energetic muons in the final state. We provide a detailed analysis of the cancellation of the related endpoint divergences appearing in individual momentum regions, and show how the rapidity logarithms can be isolated by suitable subtractions applied to the corresponding bare factorization theorem. This allows us to include in a straightforward manner the QCD corrections arising from the renormalization-group running of the hard matching coefficient of the electromagnetic dipole operator in soft-collinear effective theory, the hard-collinear scattering kernel, and the $B_s$-meson distribution amplitude. Focusing on the contribution from the double endpoint logarithms, we derive a compact formula that resums the leading-logarithmic QCD corrections.Comment: 33 pages, 3 figure

Dispersive analysis of B → K (*) and B s → ϕ form factors

We propose a stronger formulation of the dispersive (or unitarity) bounds à la Boyd-Grinstein-Lebed (BGL), which are commonly applied in analyses of the hadronic form factors for B decays. In our approach, the existing bounds are split into several new bounds, thereby disentangling form factors that are jointly bounded in the common approach. This leads to stronger constraints for these objects, to a significant simplification of our numerical analysis, and to the removal of spurious correlations among the form factors. We apply these novel bounds to B¯→K¯∗ and B¯s→ϕ form factors by fitting them to purely theoretical constraints. Using a suitable parametrization, we take into account the form factors’ below-threshold branch cuts arising from on-shell B¯sπ0 and B¯sπ0π0 states, which so-far have been ignored in the literature. In this way, we eliminate a source of hard-to-quantify systematic uncertainties. We provide machine readable files to obtain the full set of the B¯→K¯∗ and B¯s→ϕ form factors in and beyond the entire semileptonic phase space

Heavy-Quark Expansion for Bˉs→Ds(∗)\bar{B}_s\to D^{(*)}_s Form Factors and Unitarity Bounds beyond the SU(3)FSU(3)_F Limit

We carry out a comprehensive analysis of the full set of $\bar{B}_q \to D_q^{(*)}$ form factors for spectator quarks $q=u,d,s$ within the framework of the Heavy-Quark Expansion (HQE) to order $\mathcal{O}(\alpha_s, 1/m_b, 1/m_c^2)$. In addition to the available lattice QCD calculations we make use of two new sets of theoretical constraints: we produce for the first time numerical predictions for the full set of $\bar{B}_s \to D_s^{(*)}$ form factors using Light-Cone Sum Rules with $B_s$-meson distribution amplitudes. Furthermore, we reassess the QCD three-point sum rule results for the Isgur-Wise functions entering all our form factors for both $q=u,d$ and $q=s$ spectator quarks. These additional constraints allow us to go beyond the commonly used assumption of $SU(3)_F$ symmetry for the $\bar B_s\to D_s^{(*)}$ form factors, especially in the unitarity constraints which we impose throughout our analysis. We find the coefficients of the IW functions emerging at $\mathcal{O}(1/m_c^2)$ to be consistent with the naive $\mathcal{O}(1)$ expectation, indicating a good convergence of the HQE. While we do not find significant $SU(3)$ breaking, the explicit treatment of $q=s$ as compared to a simple symmetry assumption renders the unitarity constraints more effective. We find that the (pseudo)scalar bounds are saturated to a large degree, which affects our theory predictions. We analyze the phenomenological consequences of our improved form factors by extracting $|V_{cb}|$ from $\bar B\to D^{(*)}\ell\nu$ decays and producing theoretical predictions for the lepton-flavour universality ratios $R(D)$, $R(D^*)$, $R(D_s)$ and $R(D_s^*)$, as well as the $\tau$- and $D_q^*$ polarization fractions for the $\bar B_q\to D_q^{(*)}\tau\nu$ modes.Comment: 16 pages, 3 figures, 7 tables, includes ancillary files; v2: minor changes to the text, conclusions unchanged, 2 missing files added, as accepted for publication in EPJ

A puzzle in Bˉ(s)0→D(s)(∗)+{π−,K−}\bar{B}_{(s)}^0 \to D_{(s)}^{(*)+} \lbrace \pi^-, K^-\rbrace decays and extraction of the fs/fdf_s/f_d fragmentation fraction

We provide updated predictions for the hadronic decays $\bar{B}_s^0\to D_s^{(*)+} \pi^-$ and $\bar{B}^0\to D^{(*)+} K^-$. They are based on $\mathcal{O}(\alpha_s^2)$ results for the QCD factorization amplitudes at leading power and on recent results for the $\bar{B}_{(s)} \to D_{(s)}^{(*)}$ form factors up to order ${\cal O}(\Lambda_{\rm QCD}^2/m_c^2)$ in the heavy-quark expansion. We give quantitative estimates of the matrix elements entering the hadronic decay amplitudes at order ${\cal O}(\Lambda_{\rm QCD}/m_b)$ for the first time. Our results are very precise, and uncover a substantial discrepancy between the theory predictions and the experimental measurements. We explore two possibilities for this discrepancy: non-factorizable contributions larger than predicted by the QCD factorization power counting, and contributions beyond the Standard Model. We determine the $f_s/f_d$ fragmentation fraction for the CDF, D0 and LHCb experiments for both scenarios.Comment: 13 pages, 4 tables: v2: minor modifications, accepted for publication in EPJ

Lepton-flavour non-universality of Bˉ→D∗ℓνˉ\bar{B}\to D^*\ell \bar\nu angular distributions in and beyond the Standard Model

We analyze in detail the angular distributions in $\bar{B}\to D^*\ell \bar\nu$ decays, with a focus on lepton-flavour non-universality. We investigate the minimal number of angular observables that fully describes current and upcoming datasets, and explore their sensitivity to physics beyond the Standard Model (BSM) in the most general weak effective theory. We apply our findings to the current datasets, extract the non-redundant set of angular observables from the data, and compare to precise SM predictions that include lepton-flavour universality violating mass effects. Our analysis shows that the current presentation of the experimental data is not ideal and prohibits the extraction of the full set of relevant BSM parameters, since the number of independent angular observables that can be inferred from data is limited to only four. We uncover a $\sim4\sigma$ tension between data and predictions that is hidden in the redundant presentation of the Belle 2018 data on $\bar{B}\to D^*\ell \bar\nu$ decays. This tension specifically involves observables that probe $e-\mu$ lepton-flavour universality. However, we find inconsistencies in these data, which renders results based on it suspicious. Nevertheless, we discuss which generic BSM scenarios could explain the tension, in the case that the inconsistencies do not affect the data materially. Our findings highlight that $e-\mu$ non-universality in the SM, introduced by the finite muon mass, is already significant in a subset of angular observables with respect to the experimental precision.Comment: 18 pages, 2 figures, 3 table

B→D1(2420)B\to D_1(2420) and B→D1′(2430)B\to D_1'(2430) form factors from QCD light-cone sum rules

We perform the first calculation of form factors in the semileptonic decays $B\!\to\! D_1(2420)\ell\nu_\ell$ and $B \to D_1^\prime (2430)\ell \nu_\ell$ using QCD light-cone sum rules (LCSRs) with $B$-meson distribution amplitudes. In this calculation the $c$-quark mass is finite. Analytical expressions for two-particle contributions up to twist four are obtained. To disentangle the $D_1$ and $D_1^\prime$ contributions in the LCSRs, we suggest a novel approach that introduces a combination of two interpolating currents for these charmed mesons. To fix all the parameters in the LCSRs, we use the two-point QCD sum rules for the decay constants of $D_1$ and $D_1^\prime$ mesons augmented by a single experimental input, that is the $B \to D_1(2420)\ell\nu_\ell$ decay width. We provide numerical results for all $B\to D_1$ and $B\to D_1^\prime$ form factors. As a byproduct, we also obtain the $D_1$- and $D_1'$-meson decay constants and predict the lepton-flavour universality ratios $R(D_1)$ and $R(D_1')$.Comment: 30 pages, 2 figures, published versio

B → D 0 ∗ B→D0∗ B\to {D}_0^{\ast } and B s → D s 0 ∗ Bs→Ds0∗ {B}_s\to {D}_{s0}^{\ast } form factors from QCD light-cone sum rules

Abstract We present the first application of QCD light-cone sum rules (LCSRs) with B (s)-meson distribution amplitudes to the B s → D s 0 ∗ $${B}_{(s)}\to {D}_{(s)0}^{\ast }$$ form factors, where D s 0 ∗ $${D}_{(s)0}^{\ast }$$ is a charmed scalar meson. We consider two scenarios for the D 0 ∗ $${D}_0^{\ast }$$ spectrum. In the first one, we follow the Particle Data Group and consider a single broad resonance D 0 ∗ 2300 $${D}_0^{\ast }(2300)$$ . In the second one, we assume the existence of two scalar resonances, D 0 ∗ 2105 $${D}_0^{\ast }(2105)$$ and D 0 ∗ 2451 $${D}_0^{\ast }(2451)$$ , as follows from a recent theoretically motivated analysis of B → Dππ decays. The B → D 0 ∗ $$B\to {D}_0^{\ast }$$ form factors are calculated in both scenarios, also taking into account the large total width of D 0 ∗ 2300 $${D}_0^{\ast }(2300)$$ . Furthermore, we calculate the B s → D s 0 ∗ $${B}_s\to {D}_{s0}^{\ast }$$ form factors, considering in this case only the one-resonance scenario with D s0(2317). In this LCSRs calculation, the c-quark mass is kept finite and the s-quark mass is taken into account. We also include contributions of the two- and three-particle distribution amplitudes up to twist-four. Our predictions for semileptonic B → D 0 ∗ ℓ ν ℓ $$B\to {D}_0^{\ast}\ell {\nu}_{\ell }$$ and B s → D s 0 ∗ ℓ ν ℓ $${B}_s\to {D}_{s0}^{\ast}\ell {\nu}_{\ell }$$ branching ratios are compared with the available data and HQET-based predictions. As a byproduct, we also obtain the D 0 ∗ $${D}_0^{\ast }$$ - and D s 0 ∗ $${D}_{s0}^{\ast }$$ -meson decay constants and predict the lepton flavour universality ratios R D 0 ∗ $$R\left({D}_0^{\ast}\right)$$ and R D s 0 ∗ $$R\left({D}_{s0}^{\ast}\right)$$