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Related papers: Quark mass relations to four-loop order

200 papers

In the paper, we study the properties of the top-quark $\overline{\rm MS}$ running mass computed from its on-shell mass by using both the four-loop $\overline{\rm MS}$-on-shell relation and the principle of maximum conformality (PMC)…

High Energy Physics - Phenomenology · Physics 2020-06-25 Xu-Dong Huang , Xing-Gang Wu , Jun Zeng , Qing Yu , Xu-Chang Zheng , Shuai Xu

New data for the total cross section $\sigma(e^+e^-\to{hadrons})$ in the charm and bottom threshold region are combined with an improved theoretical analysis, which includes recent four-loop calculations, to determine the short distance…

High Energy Physics - Phenomenology · Physics 2008-11-26 Johann H. Kuehn , Matthias Steinhauser , Christian Sturm

We compute the two-loop term in the perturbation series for the quark-mass in the lattice Heavy Quark Effective Theory. This is an ingredient in the matching factor required to obtain the $b$-quark mass from lattice simulations of the HQET.…

High Energy Physics - Lattice · Physics 2009-10-09 G. Martinelli , C. T. Sachrajda

New results at four-loop order in perturbative QCD for the first two Taylor coefficients of the heavy quark vacuum polarization function are presented. They can be used to perform a precise determination of the charm- and bottom-quark mass.…

High Energy Physics - Phenomenology · Physics 2009-01-07 K. G. Chetyrkin , J. H. Kühn , C. Sturm

We present the results for two-loop MSSM corrections to the relation between pole and running masses of heavy quarks up to the order O(as^2). The running masses are defined in the DR scheme, usually used in multiloop calculations in…

High Energy Physics - Phenomenology · Physics 2009-01-07 A. Bednyakov , A. Onishchenko , V. Velizhanin , O. Veretin

Far above threshold the production process e^+e^-to t t-bar can be analyzed using effective field theories. In this talk we consider the invariant mass distribution of top-jets and report about our computation of the two-loop heavy quark…

High Energy Physics - Phenomenology · Physics 2009-04-14 Ambar Jain , Ignazio Scimemi , Iain W. Stewart

We compute the two-loop heavy quark jet-function in the heavy quark limit. This is one of the key ingredients in next-to-next-to-leading order (NNLO) and next-to-next-to-leading-log order (NNLL) computations of the invariant mass…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ambar Jain , Ignazio Scimemi , Iain W. Stewart

Quark masses are of great prominence in high-energy physics. In this paper, we have studied the heavy meson systems via solving the Lippmann-Schwinger equation by using the Martin potential for heavy quark masses. We have also attempted to…

High Energy Physics - Phenomenology · Physics 2015-08-04 N. Tazimi , M. Monemzadeh , M. R. Hadizadeh

Recent calculations of heavy quark cross sections near threshold at next-to-next-to-leading order have found second-order corrections as large as first-order ones. We analyse long-distance contributions to the heavy quark potential in…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Beneke

The paper is devoted to the calculation of additional two-loop O(\alpha_s^2) MSSM corrections to the relation between the pole mass of the t-quark and its running mass in the DR scheme. The value of the second order contribution from large…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Bednyakov , D. I. Kazakov , A. Sheplyakov

We compute the relation between the pole quark mass and the minimally subtracted quark mass in the framework of QCD applying dimensional reduction as a regularization scheme. Special emphasis is put on the evanescent couplings and the…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. Marquard , L. Mihaila , J. H. Piclum , M. Steinhauser

We compute the relation between the quark mass defined in the minimal modified $\MSbar$ scheme and the mass defined in the ``Regularization Invariant" scheme (RI), up to the NNLO order. The RI scheme is conveniently adopted in lattice QCD…

High Energy Physics - Phenomenology · Physics 2009-10-31 E. Franco , V. Lubicz

We consider the on-shell mass and wave function renormalization constants $Z_m^{\rm OS}$ and $Z_2^{\rm OS}$ up to three-loop order allowing for a second non-zero quark mass. We obtain analytic results in terms of harmonic polylogarithms and…

High Energy Physics - Phenomenology · Physics 2020-10-28 Matteo Fael , Kay Schönwald , Matthias Steinhauser

The study of heavy-light meson masses should provide a way to determine renormalized quark masses and other properties of heavy-light mesons. In the context of lattice QCD, for example, it is possible to calculate hadronic quantities for…

High Energy Physics - Phenomenology · Physics 2018-02-14 N. Brambilla , J. Komijani , A. S. Kronfeld , A. Vairo

We review algorithmic methods for two-loop calculations in HQET, and the analogous methods for on-shell QCD, needed for matching HQET to QCD.

High Energy Physics - Phenomenology · Physics 2007-05-23 D. J. Broadhurst , A. G. Grozin

We present the analytical calculation of the four-loop quark mass anomalous dimension in Quantum Chromodynamics within the minimal subtraction scheme. On the basis of this result we find that the so-called invariant quark mass is a very…

High Energy Physics - Phenomenology · Physics 2009-10-30 J. A. M. Vermaseren , S. A. Larin , T. van Ritbergen

The paper is devoted to the calculation of the two-loop O(alpha_s y^2) and O(y^4) MSSM corrections to the relation between the pole mass of the b-quark and its running mass in DR scheme. To evaluate the needed diagrams the large mass…

High Energy Physics - Phenomenology · Physics 2011-01-27 A. Bednyakov , A. Sheplyakov

With the increasing experimental precision available at colliders, higher-order perturbative calculations are required to reduce the theory uncertainty in order to extract crucial QCD parameters, such as the strong coupling constant, to the…

High Energy Physics - Phenomenology · Physics 2022-08-15 Marco Saragnese

Finite energy QCD sum rules involving both inverse and positive moment integration kernels are employed to determine the bottom quark mass. The result obtained in the $\bar{\text {MS}}$ scheme at a reference scale of $10\, {GeV}$ is…

High Energy Physics - Phenomenology · Physics 2015-06-03 S. Bodenstein , J. Bordes , C. A. Dominguez , J. Penarrocha , K. Schilcher

The features of the ordinary least squares method, which gives a possible way to a solution of the overdetermined systems of algebraic equations and allows to estimate the uncertainties of the obtained solutions, are considered. As the…

High Energy Physics - Phenomenology · Physics 2019-10-23 A. L. Kataev , V. S. Molokoedov