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Related papers: Precise Determinations of the Charm Quark Mass

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We investigate in detail the sensitivity of the fourth-order charm fluctuation, calculated on the lattice, to the input bare charm quark mass. We approach its continuum limit by employing four different lines of constant physics. We…

High Energy Physics - Lattice · Physics 2025-03-25 Sipaz Sharma

The physics of charm has become one of the best laboratories exposing the limitations of the naive constituent quark model and also giving hints into a more mature description of meson spectroscopy, beyond the simple quark--antiquark…

High Energy Physics - Phenomenology · Physics 2009-05-04 J. Vijande , A. Valcarce , J. -M. Richard , N. Barnea

Progress in charm physics has been prodigious over the last twenty years; it comes both from fixed target and collider experiments, and can guide us toward future investigations. To fully exploit the power of flavor physics, complications…

High Energy Physics - Experiment · Physics 2007-05-23 Sandra Malvezzi

I discuss the results of a new calculation of the charm and bottom quark masses in the quenched approximation and in the continuum limit of lattice QCD. The work has been done by the APE group at the ``Tor Vergata'' University making use of…

High Energy Physics - Lattice · Physics 2009-11-10 Nazario Tantalo

Precision results on the leptonic, semileptonic, and hadronic decays of charm mesons are reviewed. These results are important for timely progress in weak flavor physics both in their own right and as checks of theoretical calculations.…

High Energy Physics - Experiment · Physics 2009-04-07 Roy A. Briere

I briefly overview the methods employed at the LHC to extract the top-quark mass, taking particular care about the theory uncertainty and the dependence on the Monte Carlo hadronization parameters.

High Energy Physics - Phenomenology · Physics 2017-11-30 Gennaro Corcella

The theory of the strong force, quantum chromodynamics, describes the proton in terms of quarks and gluons. The proton is a state of two up quarks and one down quark bound by gluons, but quantum theory predicts that in addition there is an…

We study the so-called extended linear sigma model for the case of four quark flavors. This model is based on global chiral symmetry and dilatation invariance and includes, besides scalar and pseudoscalar mesons, vector and axial-vector…

High Energy Physics - Phenomenology · Physics 2015-09-23 Walaa I. Eshraim , Francesco Giacosa , Dirk H. Rischke

We present a study of charm physics using RBC/UKQCD 2+1 flavour physical point domain wall fermion ensembles for the light quarks as well as for the valence charm quark. After a brief motivation of domain wall fermions as a suitable heavy…

The status of lattice determinations of quark masses is reviewed (with the exception of m_b). Attempts to extract the low-energy constants in the effective chiral Lagrangian are discussed, with special emphasis on those couplings which are…

High Energy Physics - Lattice · Physics 2009-11-07 Hartmut Wittig

The uncertainty of the theoretical prediction of the $\bar B \to X_s \gamma$ branching ratio at NLL level is dominated by the charm mass renormalization scheme ambiguity. In this paper we calculate those NNLL terms which are related to the…

High Energy Physics - Phenomenology · Physics 2011-01-05 H. M. Asatrian , C. Greub , A. Hovhannisyan , T. Hurth , V. Poghosyan

We present preliminary results of an ongoing lattice QCD computation of the spectrum of $D$ mesons and $D_s$ mesons and of charmonium using 2+1+1 flavors of twisted mass sea and valence quarks.

High Energy Physics - Lattice · Physics 2013-09-12 Martin Kalinowski , Marc Wagner

We estimate the effects on the decay constants of charmonium and on heavy meson masses due to the charm quark in the sea. Our goal is to understand whether for these quantities $N_f=2+1$ lattice QCD simulations provide results that can be…

High Energy Physics - Lattice · Physics 2021-11-03 Salvatore Cali , Kevin Eckert , Jochen Heitger , Francesco Knechtli , Tomasz Korzec

We present a brief review of current methods for the calculation of multi-loop amplitudes including recent developments. As an example we present the calculation of the second moment of the heavy quark current correlator and the extraction…

High Energy Physics - Phenomenology · Physics 2008-10-21 P. Marquard

In this note we provide a detailed derivation of the kinematic limit of the charm production in fixed-target experiments with the intrinsic charm coming from the target. In addition, we discuss the first measurement of charm quark…

High Energy Physics - Phenomenology · Physics 2019-04-10 Stefan Groote , Sergey Koshkarev

We review the weak-decay and spectroscopy properties of baryons with two charmed quarks. We also present the convergent speculations on exotic mesons $(QQ\bar{q}\bar{q})$ with two heavy quarks and two light antiquarks.

High Energy Physics - Phenomenology · Physics 2007-05-23 Jean-Marc Richard

In this work the charm and bottom quark masses are determined from QCD moment sum rules for the charmonium and upsilon systems. To illustrate the special character of these sum rules when applied to Coulomb systems we first set up and study…

High Energy Physics - Phenomenology · Physics 2008-11-26 Markus Eidemuller

This paper is aimed at giving a complete review of the latest (post-1998 Physics in Collision conference) experimental results on charm physics.

High Energy Physics - Experiment · Physics 2016-11-23 Stefano Bianco

We determine the strong coupling $\alpha_s(m_Z)$ from dimensionless ratios of roots of moments of the charm- and bottom-quark vector and charm pseudo-scalar correlators, dubbed…

High Energy Physics - Phenomenology · Physics 2020-04-22 Diogo Boito , Vicent Mateu

We report on the status of the determination of the heavy quark masses from our calculation of the quarkonia spectra. All sources of systematic errors that enter the quark mass determination are accounted for. We explicitly keep $ma \neq 0$…

High Energy Physics - Lattice · Physics 2010-11-19 Aida X. El-Khadra , B. P. Mertens
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