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Related papers: Recent progress on HQET lagrangian

200 papers

We present the coefficient of the chromomagnetic interaction operator, the only unknown coefficient in the Heavy Quark Effective Theory (HQET) lagrangian up to the $1/m$ level, with the two-loop accuracy by matching scattering amplitudes of…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Czarnecki , A. G. Grozin

We present a calculation of the renormalized HQET Lagrangian at order O(1/m_Q^3) in the one particle sector. The anomalous dimensions of local operators and time ordered products of dimension 7 contributing at this order are calculated in…

High Energy Physics - Phenomenology · Physics 2016-08-25 Christopher Balzereit

We proposed a new formulation for heavy quark effective theory (HQET), whose Lagrangian is hermitian and has a manifest reparameterization invariance. As an application, we calculated the semileptonic and nonleptonic inclusive heavy hadron…

High Energy Physics - Phenomenology · Physics 2007-05-23 Tsung-Wen Yeh

We compute the three-loop QCD corrections to the quark chromomagnetic moment and thus obtain the matching coefficient and the anomalous dimension of the chromomagnetic interaction in HQET. As a byproduct we obtain the three-loop corrections…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. G. Grozin , P. Marquard , J. H. Piclum , M. Steinhauser

We present a new calculation of the renormalized HQET Lagrangian at order O(1/m_Q^2) and discuss the consequences of the BRST invariance of QCD and the reparameterization invariance of HQET. Our result corrects earlier, conflicting…

High Energy Physics - Phenomenology · Physics 2009-10-28 Christopher Balzereit , Thorsten Ohl

The operator mixing matrix for the dimension six operators in the heavy quark effective theory Lagrangian is computed at one loop. The results are shown to be consistent with constraints from the equations of motion, and from…

High Energy Physics - Phenomenology · Physics 2009-10-30 Christian Bauer , Aneesh V. Manohar

After a brief introduction to Heavy Quark Effective Theory, we discuss $\alpha$ representation in HQET and methods of calculation of some kinds of HQET diagrams up to three loops.

High Energy Physics - Phenomenology · Physics 2008-12-12 A. G. Grozin

The perturbative contribution to the correlator of two HQET heavy-light currents expanded in light-quark masses up to quadratic terms is calculated up to 4 loops. The leading large-$\beta_0$ limit is also considered, so that terms with the…

High Energy Physics - Phenomenology · Physics 2026-03-09 Andrey G. Grozin

We take the Lagrangian of Inert Doublet Model and with unitary gauge calculate all the possible interactions, after calculating the interactions we draw the corresponding Feynman diagrams.There after calculate the Scattering cross section…

High Energy Physics - Phenomenology · Physics 2023-01-13 Sumit Satapathy

We give an introduction to Heavy Quark Effective Theory (HQET). Our emphasis is on its formulation non-perturbative in the strong coupling, including the non-perturbative determination of the parameters in the HQET Lagrangian. In a second…

High Energy Physics - Lattice · Physics 2015-01-14 Rainer Sommer

We present the three-loop QCD corrections to the quark chromomagnetic moment including two different nonzero masses. This is a necessary ingredient to obtain the corresponding corrections to the chromomagnetic coefficient in the Heavy Quark…

High Energy Physics - Phenomenology · Physics 2009-06-02 S. Bekavac , A. Grozin , D. Seidel , M. Steinhauser

We determine non-perturbatively the parameters of the lattice HQET Lagrangian and those of the time component of the heavy-light axial-vector current in the quenched approximation. The HQET expansion includes terms of order 1/m. Our results…

High Energy Physics - Lattice · Physics 2014-11-20 Benoît Blossier , Michele Della Morte , Nicolas Garron , Rainer Sommer

In this talk we review recent perturbative and non-perturbative developments in Heavy Quark Effective Theory (HQET).

High Energy Physics - Phenomenology · Physics 2024-12-17 Gil Paz

The perturbative contribution to the correlator of two heavy-light quark currents in HQET expanded in light-quark masses up to quadratic terms is calculated at the leading order in $1/\beta_0$. Ultraviolet and infrared renormalon poles of…

High Energy Physics - Phenomenology · Physics 2026-04-13 Andrey G. Grozin

We complete the one loop renormalization of the HQET lagrangian at O(1/m_Q^3) including four fermion operators with two heavy and two light quark fields in the operator basis. It is shown that as a consequence the short distance…

High Energy Physics - Phenomenology · Physics 2016-08-25 Christopher Balzereit

The HQET/NRQCD Lagrangian is computed to order alpha/m^3. The computation is performed using dimensional regularization to regulate the ultraviolet and infrared divergences. The results are consistent with reparametrization invariance to…

High Energy Physics - Phenomenology · Physics 2016-08-24 Aneesh Manohar

The effect of non-zero c quark mass on b quark HQET Lagrangian, up to 1/m_b level, is calculated at two loops. The results are expressed in terms of dilogarithmic functions of m_c/m_b. This calculation involves on-shell two-loop…

High Energy Physics - Phenomenology · Physics 2011-01-25 A. I. Davydychev , A. G. Grozin

We use Heavy Quark Effective Theory (HQET) techniques to parametrize certain non-perturbative effects related to quantum fluctuations that put both heavy quark and antiquark in quarkonium almost on shell. The large off-shell momentum…

High Energy Physics - Phenomenology · Physics 2016-09-01 A. Pineda , J. Soto

We discuss how reparameterization invariance connects a rotationally-invariant heavy particle effective theory with a single fermion to a Lorentz-invariant theory. Using Hilbert-series methods, a Lorentz-invariant operator basis is…

High Energy Physics - Phenomenology · Physics 2020-01-08 Andrew Kobach , Sridip Pal

We examine the constraints imposed by reparametrization invariance on heavy-baryon chiral perturbation theory (HBChPT). We study the case of 3 flavors and consider both the strong and weak ($|\Delta S| =1$) interaction sector. Some of the…

High Energy Physics - Phenomenology · Physics 2009-10-30 J. W. Bos , D. Chang , S. C. Lee , Y. C. Lin , H. H. Shih
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