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Related papers: B -> D* at zero recoil revisited

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The weak form factor for $B\to K_{1B}$ where $K_{1B}$ is the $^1P_1$ state is calculated in the light-cone sum rules (LCSR). Combining the quark model result for the form factor of $B\to K_{1A}$ with $K_{1A}$ being the $^3P_1$ state, we…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jong-Phil Lee

The strong form factor of the $B_{c} B_{c}J/\Psi$ vertex is calculated in the framework of the QCD sum rules method at finite temperature. Taking into account additional operators appearing at finite temperature, thermal Wilson expansion is…

High Energy Physics - Phenomenology · Physics 2016-10-28 E. Yazici , H. Sundu , E. Veli Veliev

The dominant theoretical uncertainty in extracting |V_td/V_ts| from the ratio of branching ratios R=B(B->(rho,omega)gamma)/B(B->K* gamma) is given by the ratio of form factors xi=T_1^{B->K*}(0)/T_1^{B->rho}(0). We re-examine xi in the…

High Energy Physics - Phenomenology · Physics 2011-03-23 Patricia Ball , Roman Zwicky

The form factors of the semileptonic $B\to \pi\pi\ell\bar\nu$ decay are calculated from QCD light-cone sum rules with the distribution amplitudes of dipion states. This method is valid in the kinematical region, where the hadronic dipion…

High Energy Physics - Phenomenology · Physics 2016-04-20 Christian Hambrock , Alexander Khodjamirian

The form factors of $B_{(s)}$ decays into P-wave excited charmed mesons (including $D^*_0(2300)$, $D_1(2430)$, $D_1(2420)$, $D^*_2(2460)$ and their strange counterparts, denoted generically as $D^{**}_{(s)}$) are systematically calculated…

High Energy Physics - Phenomenology · Physics 2023-08-31 Ya-Bing Zuo , Hong-Yao Jin , Jing-Ying Tian , Jia Yi , Han-Yu Gong , Ting-Ting Pan

We present the status of our ongoing calculation of the zero-recoil form factor for the semileptonic decay $\bar{B}^0\rightarrow D^{*+}l^-\bar{\nu}$ using lattice QCD with 2+1+1 flavours of highly improved staggered quarks in the sea (the…

High Energy Physics - Lattice · Physics 2017-01-11 Judd Harrison , Christine Davies , Matthew Wingate

Considering the gluon condensate corrections, the form factors relevant to the semileptonic rare $B_c \rar D,D_s(J^{P}=0^{-}) l^{+}l^{-}$ with $l=\tau,\mu,e$ and $B_c \rar D,D_s(J^{P}=0^{-})\nu\bar{\nu}$ transitions are calculated in the…

High Energy Physics - Phenomenology · Physics 2008-11-26 K. Azizi , R. Khosravi

We use QCD sum rules to analyze the semileptonic transition $B \to \pi \ell \nu$ in the limit $m_b \to \infty$. We derive the dependence of the form factor $F_1(0)$ on the heavy quark mass, which is compatible with the expected dependence…

High Energy Physics - Phenomenology · Physics 2010-11-01 P. Colangelo , P. Santorelli

We present the Non-Relativistic QCD (NRQCD) calculations at the next-to-leading order (NLO) of $\alpha_s$ for $B_c^*\to \eta_c$ vector, axial-vector, tensor and axial-tensor form factors, and obtain complete analytical expressions for the…

High Energy Physics - Phenomenology · Physics 2026-03-18 Wei Tao , Ya-Hui Zhao , Li-Ting Wang , Qin Chang , Zhen-Jun Xiao

We provide a model-independent framework for the analysis of the radiative B-meson decays B -> K* gamma and B -> rho gamma. In particular, we give a systematic discussion of the various contributions to these exclusive processes based on…

High Energy Physics - Phenomenology · Physics 2010-05-28 Stefan W. Bosch , Gerhard Buchalla

We present a lattice QCD calculation of $B\to \pi l \nu$ semileptonic decay form factors in the small pion recoil momentum region. The calculation is performed on a quenched $16^3 \times 48$ lattice at $\beta=5.9$ with the NRQCD action…

In this paper, the strong form factors and coupling constants of $D_sDK^*$ and $D_sD^*K^*$ vertices are investigated within the three-point QCD sum rules method with and without the $SU_{f}(3)$ symmetry. In this calculation, the…

High Energy Physics - Phenomenology · Physics 2018-09-05 M. Janbazi , R. Khosravi

We present the result of lattice QCD calculation of the scalar, vector and tensor form factors for the $B\to K\ell^+\ell^-$ decay, across the full physical range of momentum transfer. We use the highly improved staggered quark (HISQ)…

High Energy Physics - Lattice · Physics 2023-02-08 W. G. Parrott , C. Bouchard , C. T. H. Davies

Recently it has been shown that in the large-recoil limit new symmetries emerge which impose various relations on form factors that parametrise the decay of heavy B mesons into light mesons. These symmetry relations are broken by radiative…

High Energy Physics - Phenomenology · Physics 2009-10-31 Th. Feldmann

The form factors and the coupling constant of the $B_s B^* K $ and $B_s B K^*$ vertices are calculated using the QCD sum rules method. Three point correlation functions are computed considering both the heavy and light mesons off-shell in…

High Energy Physics - Phenomenology · Physics 2015-05-20 A. Cerqueira , B. Osório Rodrigues , M. E. Bracco , M. Nielsen

We discuss threshold resummation in radiative and charmless semileptonic B decays. To deal with the large non perturbative effects, we introduce a model for NNLL resummed form factors based on the analytic QCD coupling. By means of this…

High Energy Physics - Phenomenology · Physics 2007-05-23 Giancarlo Ferrera

In this paper, we study the non-leptonic $B_{c}\to J/\psi V$ and $B_{c}^{*}\to\eta_{c}V$~$(V=\rho\,,K^{*})$ weak decays in the framework of QCD factorization. In the evaluation, the form factors are calculated by using the…

High Energy Physics - Phenomenology · Physics 2018-07-04 Qin Chang , Li-Li Chen , Shuai Xu

We present the first preliminary results for the semileptonic form factor $h_{A_1}(w=1)/\rho_{A_j}$ at zero recoil for the $\bar B \rightarrow D^\ast \ell \bar \nu$ decay using lattice QCD with four flavors of sea quarks. We use the HISQ…

High Energy Physics - Lattice · Physics 2017-11-08 Jon A. Bailey , Tanmoy Bhattacharya , Rajan Gupta , Yong-Chull Jang , Weonjong Lee , Jaehoon Leem , Sungwoo Park , Boram Yoon

We compute the vector meson decay constants fD*, fDs* from the simulation of twisted mass QCD on the lattice with Nf = 2 dynamical quarks. When combining their values with the pseudoscalar D(s)-meson decay constants, we were able (i) to…

High Energy Physics - Lattice · Physics 2015-06-03 Damir Becirevic , Vittorio Lubicz , Francesco Sanfilippo , Silvano Simula , Cecilia Tarantino

A relation among the form factors of $<D \mid A_\mu \mid D^*>$ at $q^2 \to 0$ is derived. It is verified to lowest order in both the $1/m_c$ expansion and the expansion in number of derivatives using the effective lagrangian that…

High Energy Physics - Phenomenology · Physics 2020-03-17 Claudio O. Dib , J. Taron