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We report on recent lattice QCD calculations of the strangeness magnetic moment of the nucleon and the nucleon electromagnetic form factors, when we allow the electromagnetic current to connect to quark loops as well as to the valence…

High Energy Physics - Lattice · Physics 2008-11-26 Anthony G. Williams

We compute the strangeness and light-quark contributions Delta s, Delta u and Delta d to the proton spin in nf=2 lattice QCD at a pion mass of about 285 MeV and at a lattice spacing a approx 0.073 fm, using the non-perturbatively improved…

We follow our previous paper on possible cosmological variation of weak scale (quark masses) and strong scale, inspired by data on cosmological variation of the electromagnetic fine structure constant from distant quasar (QSO) absorption…

High Energy Physics - Phenomenology · Physics 2016-09-06 V. V. Flambaum , E. V. Shuryak

Several parameters characterizing the strangeness content of the nucleon have been calculated in the chiral constituent quark model with configuration mixing (\chiCQM_{config}) which is known to provide a satisfactory explanation of the…

High Energy Physics - Phenomenology · Physics 2007-10-19 Harleen Dahiya , Manmohan Gupta

Lattice calculations of the mass of the strange quark are reviewed. In particular, the reason for the spread in values is explained with emphasis on the effects that recently implemented improvements have had on the lattice determinations.

High Energy Physics - Phenomenology · Physics 2007-05-23 Sinead Ryan

We consider the possibility that Dirac neutrino masses may be a manifestation of chiral symmetry breaking via non-perturbative QCD dynamics. The key role played by light quarks in this mechanism can naturally lead to signals that are…

High Energy Physics - Phenomenology · Physics 2022-05-19 Hooman Davoudiasl , Ian M. Lewis , Matthew Sullivan

The strange quark mass is determined from a new QCD Finite Energy Sum Rule (FESR) optimized to reduce considerably the systematic uncertainties arising from the hadronic resonance sector. As a result, the main uncertainty in this…

High Energy Physics - Phenomenology · Physics 2009-01-06 Cesareo A. Dominguez , Nasrallah F. Nasrallah , Raoul Röntsch , Karl Schilcher

We determine the strange and light quark condensates in full lattice QCD for the first time. This is done by direct calculation of the expectation value of the trace of the quark propagator followed by subtraction of the appropriate…

High Energy Physics - Lattice · Physics 2013-01-31 C. T. H. Davies , C. McNeile , A. Bazavov , R. J. Dowdall , K. Hornbostel , G. P. Lepage , H. Trottier

We present an improved determination of the strange quark and anti-quark parton distribution functions of the proton by means of a global QCD analysis that takes into account a comprehensive set of strangeness-sensitive measurements:…

High Energy Physics - Phenomenology · Physics 2021-05-04 Ferran Faura , Shayan Iranipour , Emanuele R. Nocera , Juan Rojo , Maria Ubiali

The contributions of strange quarks to the nucleon mass and the nucleon spin are investigated in a mixed action scheme employing domain wall valence quarks and quark loops on MILC asqtad dynamical fermion ensembles. Results are presented…

High Energy Physics - Lattice · Physics 2011-08-19 Michael Engelhardt

Intrinsic strangeness contributions to low-energy strange quark matrix elements of the nucleon are modelled using kaon loops and meson-nucleon vertex functions taken from nucleon-nucleon and nucleon-hyperon scattering. A comparison with…

High Energy Physics - Phenomenology · Physics 2014-11-17 M. J. Musolf , M. Burkardt

The strange-quark occupation factor ($\gamma_s$) is determined from the statistical fit of the multiplicity ratio $\mathrm{K}^+/\pi^+$ in a wide range of nucleon-nucleon center-of-mass energies ($\sqrt{s_{NN}}$). From this…

The HERMES collaboration in Phys. Rev. D89 (2014) 097101 extracted information about the strange quark density in the nucleon. One of the main results is an observation that the shape of the extracted density is very different from the…

High Energy Physics - Experiment · Physics 2015-11-25 M. Stolarski

We revisit the classical relation between the strangeness content of the nucleon, the pion-nucleon sigma term and the $SU(3)_F$ breaking of the baryon masses in the context of Lorentz covariant chiral perturbation theory with explicit…

High Energy Physics - Phenomenology · Physics 2014-02-18 J. M. Alarcon , L. S. Geng , J. Martin Camalich , J. A. Oller

The strange form factors of the nucleon are studied in a two-component model consisting of a three-quark intrinsic structure surrounded by a meson cloud. A comparison with the available experimental world data from the SAMPLE, PVA4, HAPPEX…

Nuclear Theory · Physics 2008-11-26 R. Bijker

The scalar heavy quark content of the nucleon, ${\cal M}_q = \bra{N} m_q \bar q q \ket{N},$ is relevant for computing the interaction of dark matter candidates with ordinary matter, while ${\cal M}_s$ is important for predicting the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Andrei Kryjevski

Strangeness plays an important role in the study of quark matter since it indicates the rate at which new particles are being produced and therefore provides information about the degree of chemical equilibration reached in heavy ion…

Nuclear Theory · Physics 2007-05-23 J. Cleymans

We calculate the nucleon strangeness $y_N$ in the chiral quark model and the meson cloud model. With the internal relation between the sigma term of $\pi$$N$ ($\sigma_{\pi N}$) and $y_N$, we present the results of $\sigma_{\pi N}$ in these…

High Energy Physics - Phenomenology · Physics 2008-11-26 Feng Huang , Fu-Guang Cao , Bo-Qiang Ma

We calculate the corrections to the strange matrix elements of the nucleon resulting from the breaking of rotational invariance on the light-cone. In the meson cloud model, the strange magnetic moment mu_S is seen to change sign once the…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Malheiro , W. Melnitchouk

Since the report of the SAMPLE Collaboration suggesting the strange-quark contribution to nucleon magnetic moments, G_M^s(0), may be greater than zero, numerous models have appeared supporting positive values for G_M^s(0). In this paper the…

Nuclear Theory · Physics 2007-05-23 Derek B. Leinweber