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Related papers: The Isgur-Wise function in a relativistic model fo…

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The heavy quark effective theory is developed on the light-front. Based on this effective theory, a light-front heavy meson bound state with definite spin and parity is constructed. Within the effective theory, the Isgur-Wise function is…

High Energy Physics - Phenomenology · Physics 2009-10-28 Chi-Yee Cheung , Wei-Min Zhang , Guey-lin Lin

Wavefunctions of a relativistic heavy quark-light quark $(Q,q)$ system described by a Dirac hamiltonian are analyzed. By assuming that the confinement potential is a Lorentz scalar (S), the slope of the Isgur-Wise function is calculated at…

High Energy Physics - Phenomenology · Physics 2009-09-25 M. Avila

We use a $1S$ lattice QCD heavy-light wavefunction to generate a single parameter, model independent description of the Isgur-Wise function. Using recent data we find the zero-recoil slope to be $\xi'(1)= -1.16\pm 0.17$, while the second…

High Energy Physics - Phenomenology · Physics 2016-09-01 M. G. Olsson , S. Veseli

We compute the Isgur-Wise function using heavy quark effective theory formulated on the lattice. The non-relativistic kinetic energy term of the heavy quark is included to the action as well as terms remaining in the infinite quark mass…

High Energy Physics - Lattice · Physics 2009-10-28 S. Hashimoto , H. Matsufuru

We use a method recently suggested for evaluating the slope of the Isgur-Wise function, at the zero-recoil point, on the lattice. The computations are performed in the quenched approximation to lattice QCD, on a $24^3 \times 48$ lattice at…

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

We calculate the Isgur-Wise function ($\xi_0$) by measuring the heavy-heavy meson transition matrix element on the lattice in the quenched approximation. The standard Wilson action is used for both the heavy and the light quarks. Our…

High Energy Physics - Lattice · Physics 2009-10-22 C. Bernard , Y. Shen , A. Soni

Sum rules based upon heavy quark effective theory indicate that the Isgur-Wise function $\xi(w)$ has a minimum slope as w approaches 1, which is zero for light degrees of freedom with zero spin and 1/4 for light spin 1/2. Quark-model…

High Energy Physics - Phenomenology · Physics 2008-02-03 B. D. Keister

Using the OPE, we obtain new sum rules in the heavy quark limit of QCD, in addition to those previously formulated. Key elements in their derivation are the consideration of the non-forward amplitude, plus the systematic use of boundary…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Le Yaouanc , L. Oliver , J. -C. Raynal

The integral representation for Isgur -- Wise function (IWF) is obtained in the framework of instant--form relativistic Hamiltonian dynamics for mesons with one heavy quark. The upper and lower limits are calculated for the slope parameter…

High Energy Physics - Phenomenology · Physics 2014-11-17 A. F. Krutov , O. I. Shro , V. E. Troitsky

In the heavy quark limit of QCD, using the Operator Product Expansion, the formalism of Falk for hadrons or arbitrary spin, and the non-forward amplitude, as proposed by Uraltsev, we formulate sum rules involving the Isgur-Wise function…

High Energy Physics - Phenomenology · Physics 2009-02-26 A. Le Yaouanc , L. Oliver , J. -C. Raynal

Using the framework of the Heavy Quark Effective Theory we have re-analyzed the Isgur-Wise function describing semileptonic \Lambda_b to \Lambda_c decays in the QCD sum rule approach. The slope parameter of the Isgur-Wise function is found…

High Energy Physics - Phenomenology · Physics 2014-11-18 Ming-Qiu Huang , Hong-Ying Jin , J. G. Körner , Chun Liu

We pursue the group theoretical method to study Isgur-Wise functions. We apply the general formalism, formerly applied to the baryon case j^P = 0^+ (for \Lambda_b -> \Lambda_c \ell \nu), to mesons with j^P = 1/2^-, i.e. $\overline{B} ->…

High Energy Physics - Phenomenology · Physics 2014-12-17 A. Le Yaouanc , L. Oliver , J. -C. Raynal

We consider the Isgur-Wise function xi(omega) within a new modified version of a heavy-light chiral quark model. While early versions of such models gave too small absolute value of the slope, namely xi'(1) of about -0.4 to -0.3, we show…

High Energy Physics - Phenomenology · Physics 2010-05-12 Jan O. Eeg , Kresimir Kumericki

We report some approximate analytic form of meson wave function constructed upon solving Schrodinger equation with linear plus Coulomb type Cornell potential. With this wave function, we study Isgur-Wise function and its derivatives for…

High Energy Physics - Phenomenology · Physics 2016-11-29 Sabyasachi Roy , D K Choudhury

The slope of the Isgur-Wise function for ground state mesons is evaluated for the heavy mass limit of quark models \`a la Bakamjian-Thomas, which has been previously discussed by us in general terms. A full calculation in various…

High Energy Physics - Phenomenology · Physics 2009-10-30 V. Morénas , A. Le Yaouanc , L. Oliver , O. Pène , J. -C. Raynal

We calculate the Isgur-Wise function on the lattice, simulating the light quark with the Wilson action and the heavy quark with a direct lattice implementation of the heavy-quark effective theory. Improved smearing functions produced by a…

High Energy Physics - Lattice · Physics 2008-11-26 Joseph Christensen , Terrence Draper , Craig McNeile

The Relativistic Flux Tube model is used to calculate of the Isgur-Wise functions describing the exclusive semileptonic decays of $\bar{B}$ and $\bar{B}_{s}$ mesons. The light quark mass dependence is investigated and the predicted…

High Energy Physics - Phenomenology · Physics 2010-11-01 M. G. Olsson , S. Veseli

The space-like elastic form factor of heavy-light pseudoscalar mesons is investigated within a light-front constituent quark model in order to evaluate the Isgur-Wise form factor. The relativistic composition of the constituent quark spins…

High Energy Physics - Phenomenology · Physics 2009-10-28 S. Simula

In a preceeding study in the heavy quark limit of QCD, it has been demonstrated that the best lower bound on the curvature of the Isgur-Wise function Xsi(w) is Xsi"(1) > (4rho2+3(rho2)2) > 15/16. The quadratic term (rho2)2 is dominant in a…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. Jugeau , A. Le Yaouanc , L. Oliver , J. -C. Raynal

From sum rules in the heavy quark limit of QCD, using the non-forward amplitude, we demonstrate that if the slope rho^2 = -xsi'(1) of the Isgur-Wise function xsi(w) attains its lower bound 3/4 (as happens in the BPS limit proposed by…

High Energy Physics - Phenomenology · Physics 2007-05-23 F. Jugeau , A. Le Yaouanc , L. Oliver , J. -C. Raynal
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