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Related papers: Strangeness and Chiral Symmetry Breaking

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The implications of chiral $SU(3)_L \times SU(3)_R$ symmetry and heavy quark symmetry for the radiative decays $D^{*0}\to D^0\gamma$, $D^{*+}\to D^+\gamma$, and $D_s^*\to D_s\gamma$ are discussed. Particular attention is paid to $SU(3)$…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. F. Amundson , C. G. Boyd , E. Jenkins , M. Luke , A. V. Manohar , J. L. Rosner , M. J. Savage , M. B. Wise

We discuss the dressing of constituent quarks with a pseudoscalar meson cloud within the effective chiral quark model. SU(3) flavor symmetry breaking effects are included explicitly. Our results are compared with those of the traditional…

Nuclear Theory · Physics 2008-11-26 Antoni Szczurek , Alfons J. Buchmann , Amand Faessler

Employing functional approaches the infrared behaviour of Landau gauge QCD vertex functions is investigated. Results for the ghost-gluon, three-gluon and quark-gluon vertex functions are presented. As can be analytically shown a linear…

High Energy Physics - Phenomenology · Physics 2008-11-26 Reinhard Alkofer , Christian S. Fischer , Felipe J. Llanes-Estrada , Kai Schwenzer

We propose a new approach to the determination of hadronic observables in which the essential features of chiral symmetry are combined with conventional constituent quark models. To illustrate the approach, we consider the simple quark…

High Energy Physics - Phenomenology · Physics 2010-02-17 I. C. Cloet , D. B. Leinweber , A. W. Thomas

The chiral quark model with a nonet of Goldstone bosons can yield an adequate description of the observed proton flavor and spin structure. In a previous publication we have compared the results of a SU(3) symmetric calculation with the…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. P. Cheng , Ling-Fong Li

The instanton approach to spontaneous chiral symmetry breaking is reviewed, with emphasis on the connection to chiral random matrix theory. We extend the approach to discuss the finite density, zero-temperature behaviour of quark matter.…

High Energy Physics - Phenomenology · Physics 2007-05-23 Gregory W. Carter , Dmitri Diakonov

The presence of strange sea quark pairs may have a significant impact of the pattern of chiral symmetry breaking : in particular large differences can occur between the chiral limits of two and three massless flavours (i.e., whether $m_s$…

High Energy Physics - Lattice · Physics 2008-11-26 S. Descotes-Genon

We impose an $S_3$ symmetry on the quark fields under which two of three quarks transform like a doublet and the remaining one as singlet, and use a scalar sector with the same structure of $SU(2)$ doublets. After gauge symmetry breaking, a…

High Energy Physics - Phenomenology · Physics 2016-01-06 Dipankar Das , Ujjal Kumar Dey , Palash B. Pal

I report on recent progress in the study of mass generation in non-abelian gauge theories, and concentrate on the origin of constituent masses in QCD. I argue that a consistent formalism has been developed to describe chiral symmetry…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. R. Cudell

In this contribution, we briefly analyze the formalism of the unquenched quark model (UQM) and its application to the description of several observables of hadrons. In the UQM, the effects of $q \bar q$ sea pairs are introduced explicitly…

Nuclear Theory · Physics 2015-09-30 Hugo García Tecocoatzi , Roelof Bijker

Two different approaches to mass and structure of the nucleon are discussed in recent works, ${\it viz.}$ (case 1) the QCD lagrangian evaluated via lattice calculations and (case ii) spontaneous symmetry breaking mediated by the $\sigma$…

High Energy Physics - Phenomenology · Physics 2019-08-26 Martin Schumacher

We establish a relationship between the scalar meson spectrum and the $U_A (1)$ symmetry-breaking 't Hooft interaction on one hand and the constituent quark's flavor-singlet axial coupling constant $g_{A, Q}^{(0)}$ on the other, using an…

High Energy Physics - Phenomenology · Physics 2008-11-26 V. Dmitrasinovic

The nucleon strange and anti-strange distribution asymmetry is an important issue in the study of the nucleon structure. In this work, we show that the heavy quark recombination processes from a perturbative QCD picture can give a sizable…

High Energy Physics - Phenomenology · Physics 2008-11-26 Puze Gao , Bo-Qiang Ma

We extend to the strange quarks and antiquarks, the statistical approach of parton distributions and we calculate the strange quark asymmetry $s-\bar s$. We find that the asymmetry is small, positive in the low $x$ region and negative in…

High Energy Physics - Phenomenology · Physics 2008-11-26 Claude Bourrely , Franco Buccella , Jacques Soffer

An examination of the symmetries manifest in the QCD path integral for current matrix elements reveals various equalities among the quark sector contributions. QCD equalities among octet baryon magnetic moments lead to a determination of…

High Energy Physics - Phenomenology · Physics 2009-10-28 Derek B. Leinweber

Strange matrix elements of the nucleon are calculated within the light-cone formulation of the meson cloud model. The $Q^2$ dependence of the strange vector and axial vector form factors is computed, and the strangeness radius and magnetic…

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

We have calculated the axial-vector form factors of the low lying octet baryons ($N$, $\Sigma$, $\Xi$ and $\Lambda$) in the chiral constituent quark model ($\chi$CQM). In particular, we have studied the implications of chiral symmetry…

High Energy Physics - Phenomenology · Physics 2015-06-22 Harleen Dahiya , Monika Randhawa

The strangeness degrees of freedom in the parton structure of the nucleon are explored in the global analysis framework, using the new CTEQ6.5 implementation of the general mass perturbative QCD formalism of Collins. We systematically…

High Energy Physics - Phenomenology · Physics 2014-11-18 H. L. Lai , P. Nadolsky , J. Pumplin , D. Stump , W. K. Tung , C. -P. Yuan

We report the correction from the asymmetric strange-antistrange sea of the nucleon by using both the light-cone baryon-meson fluctuation model and the chiral quark model, and show that a significant part of the NuTeV anomaly can be…

High Energy Physics - Phenomenology · Physics 2009-11-11 Bo-Qiang Ma

The strange and antistrange quark distributions of the nucleon are less constrained by experimental data than the non-strange quark sea. The combination of light quark sea distributions, $\Delta(x)=\dbar(x)+\ubar(x)-s(x)-\sbar(x)$,…

High Energy Physics - Phenomenology · Physics 2010-08-26 H. Chen , F. -G. Cao , A. I. Signal
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