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Related papers: The charm quark mass from non-relativistic sum rul…

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We provide a new determination of the charm quark mass using the Highly Improved Staggered Quark (HISQ) action, finding m_c(3 GeV) = 0.983(23) GeV. Our determination makes extensive use of second order lattice perturbation theory in…

High Energy Physics - Lattice · Physics 2019-08-13 I. F. Allison , K. Y. Wong , C. T. H. Davies , C. McNeile , H. D. Trottier , E. Dalgic , J. Wu , E. Follana , R. R. Horgan , G. P. Lepage , J. Shigemitsu

We update the experimental moments for the charm quark as computed in arXiv:hep-ph/0702103. and used in arXiv:0907.2110 and arXiv:1010.6157 for the determination of the charm-quark mass. The new value for the MSbar charm-quark mass reads…

High Energy Physics - Phenomenology · Physics 2017-12-13 Konstantin G. Chetyrkin , Johann H. Kuhn , Andreas Maier , Philipp Maierhofer , Peter Marquard , Matthias Steinhauser , Christian Sturm

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

The mass of the bottom quark can be determined with high precision from moments of the pair-production cross section sigma(e+ e- -> b bbar) near threshold. We present the first complete NNNLO determination from non-relativistic sum rules,…

High Energy Physics - Phenomenology · Physics 2016-01-14 Martin Beneke , Andreas Maier , Jan Piclum , Thomas Rauh

The mass of the charm quark is analyzed in the context of QCD finite energy sum rules using recent BESII e+e- annihilation data and a large momentum expansion of the QCD correlator which incorporates terms to order (alpha_s)^2…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. Penarrocha , K. Schilcher

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

Using new four-loop results for the heavy quark vacuum polarization and new data for bottom quark production in electron-positron annihilation, an update on the determination of charm- and bottom-quark masses through sum rules has been…

High Energy Physics - Phenomenology · Physics 2015-02-11 K. G. Chetyrkin , J. H. Kuhn , A. Maier , P. Maierhöfer , P. Marquard , M. Steinhauser , C. Sturm

We present new determinations of the MS-bar charm quark mass using relativistic QCD sum rules at O(alpha_s^3) from the moments of the vector and the pseudoscalar current correlators. We use available experimental measurements from e+e-…

High Energy Physics - Phenomenology · Physics 2015-09-02 Bahman Dehnadi , Andre H. Hoang , Vicent Mateu

In this talk we discuss results of a new extraction of the MS-bar charm quark mass using relativistic QCD sum rules at O(as**3) based on moments of the vector and the pseudoscalar current correlators and using the available experimental…

High Energy Physics - Phenomenology · Physics 2014-11-21 Bahman Dehnadi , Andre H. Hoang , Vicent Mateu

I review recent determinations of the (on-shell) charm- and beauty-quark masses in the framework of relativistic and non-relativistic ratios of Laplace transform QCD moment sum rules. The validity of the non-relativistic version of QCD sum…

High Energy Physics - Phenomenology · Physics 2007-05-23 C. A. Dominguez

We present a lattice determination of the charm quark's mass, using the mass of the D_s meson as experimental input. All errors are under control with the exception of the quenched approximation. Setting the scale with F_K=160 MeV, our…

High Energy Physics - Phenomenology · Physics 2009-11-07 Juri Rolf , Stefan Sint

The running charm-quark mass in the $\bar{MS}$ scheme is determined from weighted finite energy QCD sum rules (FESR) involving the vector current correlator. Only the short distance expansion of this correlator is used, together with…

High Energy Physics - Phenomenology · Physics 2010-12-28 S. Bodenstein , J. Bordes , C. A. Dominguez , J. Peñarrocha , K. Schilcher

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

A finite-energy sum-rule is presented that allows for the use of combinations of both positive- and inverse-moment integration kernels. The freedom afforded from being able to employ this large class of integration kernels in our sum-rule…

High Energy Physics - Phenomenology · Physics 2015-06-16 S. Bodenstein

We update determination of the $\overline{\rm MS}$ masses of the charm and bottom quarks, from comparisons of the masses of the charmonium and bottomonium $1S$ states with their perturbative predictions up to next-to-next-to-next-to-leading…

High Energy Physics - Phenomenology · Physics 2017-03-23 Yuichiro Kiyo , Go Mishima , Yukinari Sumino

Recent theoretical and experimental improvements in the determination of charm and bottom quark masses are discussed. The final results, $m_c(3 \text{GeV})=986(13) $MeV and $m_b(m_b)=4163(16) $MeV represent, together with a closely related…

High Energy Physics - Phenomenology · Physics 2010-01-29 Johann H. Kuhn

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

We study the shift in the $\Upsilon$ mass due to a non-zero charm quark mass. This shift affects the value of the $\bar{\rm MS}$ $b$-quark mass extracted from the $\Upsilon$ system by about -20 MeV, due to an incomplete cancellation of…

High Energy Physics - Phenomenology · Physics 2011-01-25 A. H. Hoang , A. V. Manohar

New data for the total cross section sigma(e^+e^- --> 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 2007-05-23 Johann H. Kuhn , Matthias Steinhauser , Christian Sturm

We present a QCD sum rule calculation of the strange-quark mass including four-loop QCD corrections to the correlator of scalar currents. We obtain $\bar m_s(1$ GeV$)=205.5\pm 19.1$ MeV.

High Energy Physics - Phenomenology · Physics 2008-11-26 K. G. Chetyrkin , D. Pirjol , K. Schilcher