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Related papers: B -> D* l nu at zero recoil: an update

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We study the vector, scalar and tensor form factors for the semileptonic process $D\rightarrow K$ by using lattice Quantum Chromodynamcs (QCD). Chiral lattice fermions are used in our study: overlap fermion for the valence quark and…

High Energy Physics - Lattice · Physics 2025-03-04 Tinghong Shen , Ying Chen , Ming Gong , Dong-Hao Li , Keh-Fei Liu , Zhaofeng Liu , Zhenyu Zhang

We explore semileptonic $B$ decays to the four lightest excited charm mesons, $D^{**} = \{D_0^*,\, D_1^*,$ $D_1,\, D_2^*\}$, for nonzero charged lepton mass and for all $b\to c \ell\bar\nu$ four-Fermi interactions, including calculation of…

High Energy Physics - Phenomenology · Physics 2018-05-07 Florian U. Bernlochner , Zoltan Ligeti , Dean J. Robinson

We report on recent progress in the calculation of $B_K$ using HYP-smeared improved staggered fermions on the MILC asqtad lattices. We have added measurements on fine ($a\sim 0.09 $fm) and superfine ($a\sim 0.06 $fm) ensembles at different…

We re-examine the determination of $|V_{cb}|$ from $B\to D \ell \nu$ in view of recent experimental and theoretical progress, discussing the parameterization of the form factors and studying the role played by the unitarity constraints. Our…

High Energy Physics - Phenomenology · Physics 2016-11-15 Dante Bigi , Paolo Gambino

The semileptonic decay channel B -> D tau nu is sensitive to the presence of a scalar current, such as that mediated by a charged-Higgs boson. Recently the BaBar experiment reported the first observation of the exclusive semileptonic decay…

We calculate semileptonic form factors for the decays $B_c \to \eta_c \, l \nu$ and $B_c \to J/\psi \, l \nu$ over the entire $q^2$ range, using a highly improved lattice quark action for charm at several lattice spacings down to $a=0.045$…

High Energy Physics - Lattice · Physics 2016-11-08 Brian Colquhoun , Christine Davies , Jonna Koponen , Andrew Lytle , Craig McNeile

Lattice calculations of the form factors for $\bar{B}\to D^{(*)}\ell\bar{\nu}$ decays can be used to extract the CKM matrix element $|V_{cb}|$. The Oktay-Kronfeld action is a highly improved version of the Fermilab action, which…

High Energy Physics - Lattice · Physics 2016-12-30 Jon A. Bailey , Jaehoon Leem , Weonjong Lee , Yong-Chull Jang

We present an update of the D meson decay constant f_D using the Highly Improved Staggered Quark (HISQ) action for valence charm and light quarks on MILC N_f = 2+1 lattices. The new determination incorporates HPQCD's improved scale r_1^{N_f…

High Energy Physics - Lattice · Physics 2013-05-30 Heechang Na , Christine T. H. Davies , Eduardo Follana , G. Peter Lepage , Junko Shigemitsu

We perform a lattice calculation on the radiative decay of $D_s^*$ using the (2+1)-flavor Wilson-clover gauge ensembles generated by CLQCD collaboration. A method allowing us to calculate the form factor with zero transfer momentum is…

High Energy Physics - Lattice · Physics 2024-04-30 Yu Meng , Jin-Long Dang , Chuan Liu , Zhaofeng Liu , Tinghong Shen , Haobo Yan , Ke-Long Zhang

We present the first three-flavor lattice QCD calculations for $D\to \pi l\nu$ and $D\to K l\nu$ semileptonic decays. Simulations are carried out using ensembles of unquenched gauge fields generated by the MILC collaboration. With an…

An explicit relativistic light-front quark model is presented which gives the momentum transfer dependent form factors of weak hadronic currents among heavy pseudoscalar and vector mesons in the whole accessible kinematic region $ 0\leq q^2…

High Energy Physics - Phenomenology · Physics 2008-02-03 N. B. Demchuk , P. Yu. Kulikov , I. M. Narodetskii , Patrick J. O'Donnell

We present results from quenched lattice QCD for the form factors for the decay $B\to\rho l\nu$. The calculations are performed using a nonperturbatively improved action and operators at two values of the lattice spacing. The bottom quark…

High Energy Physics - Lattice · Physics 2011-01-27 K. C. Bowler , J. F. Gill , C. M. Maynard , J. M. Flynn

We calculate the form factors for the semileptonic decays $B_s\to K\ell\nu$ and $B\to K\ell\ell$ with lattice QCD. We work at several lattice spacings and a range of light quark masses, using the MILC 2+1-flavor asqtad ensembles. We use the…

Dispersive constraints on the shape of the form factors which describe the exclusive decays B -> D^(*) l nu are derived by fully exploiting spin symmetry in the ground-state doublet of heavy-light mesons. The analysis includes all twenty…

High Energy Physics - Phenomenology · Physics 2009-10-30 I. Caprini , L. Lellouch , M. Neubert

We report on the advances in our unquenched calculation of the matrix elements relevant for the analysis of B^0-\bar B^0 mixing using the Asqtad (light quark) and Fermilab (heavy quark) actions. We have calculated the hadronic parameters…

High Energy Physics - Lattice · Physics 2010-11-19 R. Todd Evans , Elvira Gamiz , Aida X. El-Khadra , Massimo Di Pierro

This paper reviews recent progress of lattice gauge theory determinations of semileptonic B and D decay form factors. These determinations are important in extracting the remaining CKM matrix elements.

High Energy Physics - Phenomenology · Physics 2007-05-23 Alan Gray

We present results of a lattice computation of the matrix elements of the vector and axial-vector currents which are relevant for the semi-leptonic decays $D \rightarrow K$ and $D \rightarrow K^*$. The computations are performed in the…

High Energy Physics - Lattice · Physics 2012-08-27 UKQCD Collaboration

The general structure of the $1/m$ corrections at zero recoil is studied. The relevant matrix elements are forward matrix elements of local higher dimensional operators and their time ordered products with higher order terms from the…

High Energy Physics - Phenomenology · Physics 2010-11-01 Thomas Mannel

We present results for the kaon mixing parameter $B_K$ obtained using improved staggered fermions on a much enlarged set of MILC asqtad lattices. Compared to our previous publication, which was based largely on a single ensemble at each of…

We analyzed two form factors $T_1(q^2)$ and $T_2(q^2)$ which enter the $B\to K^* \ell^+ \ell^-$ decay rate and are accessible in the lattice calculations for $B \to K^* \gamma$. The extrapolation to $q^2=0$, necessary for $B\to K^* \gamma$…

High Energy Physics - Phenomenology · Physics 2007-05-23 Damir Becirevic
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