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Related papers: Charm and Bottom Quark Masses: an Update

200 papers

We compute charm and bottom quark masses in the quenched approximation and in the continuum limit of lattice QCD. We make use of a step scaling method, previously introduced to deal with two scale problems, that allows to take the continuum…

High Energy Physics - Lattice · Physics 2016-09-01 G. M. de Divitiis , M. Guagnelli , F. Palombi , R. Petronzio , N. Tantalo

We present a determination of the charm-quark mass in the MSbar scheme using the data combination of charm production cross section measurements in deep-inelastic scattering at HERA. The framework of global analyses of the proton structure…

High Energy Physics - Phenomenology · Physics 2015-06-12 S. Alekhin , J. Blumlein , K. Daum , K. Lipka , S. Moch

The meaning and the extraction of heavy quark masses are discussed. A simple production model is presented which incorporates the running of the heavy quark mass into perturbative calculations. The model offers the possibilities of (i)…

High Energy Physics - Phenomenology · Physics 2007-05-23 Thomas J. Weiler , K. Ghafoori--Tabrizi

We use the threshold expansion and non-relativistic effective theory to determine the bottom quark mass from moments of the $b\bar{b}$ production cross section at next-to-next-to-leading order in the (resummed) perturbative expansion, and…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Beneke , A. Signer , V. A. Smirnov

Recent results for charm quark mass effects in perturbative bottom quark mass determinations from $\Upsilon$ mesons are reviewed. The connection between the behavior of light quark mass corrections and the infrared sensitivity of some…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. H. Hoang

The charm quark's mass is determined from Monte Carlo calculations of the $\bar{c}c$ spectrum. The main sources of uncertainty are perturbation theory (for conversion to $\MSbar$), the continuum-limit extrapolation, Monte Carlo statistics,…

High Energy Physics - Lattice · Physics 2008-11-26 Andreas S. Kronfeld

We report on the result for the charm quark mass as obtained from our lattice QCD computation in the quenched approximation. Our result in the MSbar scheme is m_c(m_c)=1.26(4)(12) GeV.

High Energy Physics - Phenomenology · Physics 2008-11-26 Damir Becirevic , Vittorio Lubicz , Guido Martinelli

The most recent recalculation of the two-loop correction to the static quark-antiquark potential gave the numerical value different from the previously known one. We comment on the effect this change produces on the numerical estimates of…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. A. Penin , A. A. Pivovarov

We approximately compute the normalization constant of the first infrared renormalon of the pole mass (and the singlet static potential). Estimates of higher order terms in the perturbative relation between the pole mass and the $\MS$ mass…

High Energy Physics - Phenomenology · Physics 2009-11-07 Antonio Pineda

We determine the charm-quark mass mc(mc) in the MS-bar scheme using measurements of charm production in deep-inelastic ep scattering at HERA in the kinematic range of photon virtuality from 5 to 1000 GeV squared and Bjorken scaling variable…

High Energy Physics - Phenomenology · Physics 2015-06-11 S. Alekhin , K. Daum , K. Lipka , S. Moch

I review the current status of lattice calculations of light and heavy quark masses. Significant progresses, in these studies, have been allowed by the introduction of improved actions and non-perturbative renormalization techniques.…

High Energy Physics - Lattice · Physics 2008-11-26 V. Lubicz

The charm-loop contribution to B -> Xs gamma is found to be numerically dominant and very stable under logarithmic QCD corrections. The strong enhancement of the branching ratio by QCD logarithms is mainly due to the b-quark mass evolution…

High Energy Physics - Phenomenology · Physics 2008-11-26 Paolo Gambino , Mikolaj Misiak

We combine the known asymptotic behaviour of the QCD perturbation series expansion, which relates the pole mass of a heavy quark to the MSbar mass, with the exact series coefficients up to the four-loop order to determine the ultimate…

High Energy Physics - Phenomenology · Physics 2017-11-22 M. Beneke , P. Marquard , P. Nason , M. Steinhauser

In this contribution two recent analyses for the extraction of the charm quark mass are discussed. Although they rely on completely different experimental and theoretical input the two methods provide the same final results for the charm…

High Energy Physics - Phenomenology · Physics 2017-08-23 Matthias Steinhauser

The bottomonium spectrum up to $n = 3$ is studied within Non-Relativistic Quantum Chromodynamics up to N$^3$LO. We consider finite charm quark mass effects both in the QCD potential and the $\overline{\mathrm{MS}}$-pole mass relation up to…

High Energy Physics - Phenomenology · Physics 2018-01-29 Vicent Mateu , Pablo G. Ortega

We present a lattice QCD calculation of the up, down, strange and charm quark masses performed using the gauge configurations produced by the European Twisted Mass Collaboration with Nf = 2 + 1 + 1 dynamical quarks, which include in the…

We present a new QCD sum rule with high sensitivity to the continuum regions of charm and bottom quark pair production. Combining this sum rule with existing ones yields very stable results for the msbar quark masses, m_c(m_c)$ and m_b…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jens Erler , Mingxing Luo

We present new values for the $\bar{MS}$ masses of $b$ and $c$ quarks based on lattice NRQCD simulations of the $\Upsilon (b\bar{b})$ and $\psi (c\bar{c})$ systems. These include three measurements of the $b$ mass based on quenched…

High Energy Physics - Lattice · Physics 2012-08-27 K. Hornbostel , in collaboration with , : , C. T. H. Davies , G. P. Lepage , C. J. Morningstar , J. Shigemitsu , J. Sloan

We update our perturbative determination of MSbar bottom quark mass mb(mb), by including the recently obtained four-loop coefficient in the relation between the pole and MSbar mass. First the renormalon subtracted (RS or RS') mass is…

High Energy Physics - Phenomenology · Physics 2016-12-21 Cesar Ayala , Gorazd Cvetic , Antonio Pineda

The determination of the charm quark mass is now possible to 1% from QCD, with lattice QCD pushing the error down below 1%. I will describe the ingredients of this approach and how it can achieve this accuracy. Results for quark mass…

High Energy Physics - Lattice · Physics 2013-12-06 Christine Davies