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Related papers: Strange Mass Corrections to Hyperonic Semi-leptoni…

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The use of weak decays to determine proton spin structure is examined in view of possible violations of the Bjorken and Gottfried Sum rules, flavor symmetry breaking and flavor asymmetry in the sea. The use of the neutron decay is found to…

High Energy Physics - Phenomenology · Physics 2009-10-28 Harry J. Lipkin

A suitable wave function for baryon decuplet is framed with inclusion of sea containing quark- gluon Fock states. Relevant operator formalism is applied to calculate magnetic moments of JP = 3 2 + baryon decuplet. Statistical model assumes…

High Energy Physics - Phenomenology · Physics 2016-05-13 Amanpreet Kaur , Alka Upadhyay

The weak vector and axial-vector form factors have been investigated for the semi-leptonic octet baryon decays in the chiral constituent quark model with configuration mixing (\chiCQM_{config}). The effects of SU(3) symmetry breaking and…

High Energy Physics - Phenomenology · Physics 2009-08-24 Harleen Dahiya , Neetika Sharma , P. K. Chatley , Manmohan Gupta

We calculate the semileptonic baryon octet-octet transition form factors using a manifestly Lorentz covariant quark model approach based on the factorization of the contribution of valence quarks and chiral effects. We perform a detailed…

High Energy Physics - Phenomenology · Physics 2010-04-15 Amand Faessler , Thomas Gutsche , Barry R. Holstein , Mikhail A. Ivanov , Jurgen G. Korner , Valery E. Lyubovitskij

We analyze the semileptonic weak decays of the octet baryons in a "model independent" approach, based on the algebraic structure of the Chiral Quark-Soliton Model. We argue that this analysis is in fact more general than the model itself.…

High Energy Physics - Phenomenology · Physics 2010-06-23 M. Praszalowicz , H. -Ch. Kim , K. Goeke

Strangeness contents of baryons are calculated within rigid rotator model for arbitrary number of colors $N_c$. The problem of extrapolation to realistic value $N_c=3$ is noted, based on explicit calculations and comparison of rigid rotator…

High Energy Physics - Phenomenology · Physics 2009-11-11 Vladimir B. Kopeliovich , Andrei M. Shunderuk

We compute the strangeness content of the baryon octet and decuplet states based on an analysis of recent lattice simulations of the BMW, PACS, LHPC and HSC groups for the pion-mass dependence of the baryon masses. Our results rely on the…

High Energy Physics - Phenomenology · Physics 2015-06-04 A. Semke , M. F. M. Lutz

We study the electromagnetic form factors of the lowest-lying singly heavy baryons in a pion mean-field approach, which is also known as the SU(3) chiral quark-soliton model. In the limit of the heavy-quark mass, the dynamics inside a…

High Energy Physics - Phenomenology · Physics 2021-02-17 June-Young Kim , Hyun-Chul Kim

In this study, we assume the hadrons as an ensemble of quark-gluon Fock states and apply statistical effects to explain the spin distribution of quarks for lambda hyperon. We extend the principle of detailed balance given by Zhang et al.…

High Energy Physics - Phenomenology · Physics 2013-07-02 M. Batra , A. Upadhyay

We consider the predictions of chiral perturbation theory for $SU(3)$ breaking in the axial vector form factor $g_1$ measured in semileptonic hyperon decays. We confirm that if only octet baryon intermediate states are included, the…

High Energy Physics - Phenomenology · Physics 2014-11-17 Markus A. Luty , Martin White

The role of zero mode quantum corrections to the energy of baryonic systems with exotic quantum numbers (strangeness) is discussed. A simple expression for the contribution depending on strange inertia is obtained in the $SU(3)-$collective…

Nuclear Theory · Physics 2016-01-26 Vladimir Kopeliovich

Using an SU(3) flavour symmetry breaking expansion in the quark mass, we determine the QCD component of the neutron-proton, Sigma and Xi mass splittings of the baryon octet due to up-down (and strange) quark mass differences. Provided the…

High Energy Physics - Lattice · Physics 2012-12-24 R. Horsley , J. Najjar , Y. Nakamura , D. Pleiter , P. E. L. Rakow , G. Schierholz , J. M. Zanotti

Using an SU(3)-flavour symmetry breaking expansion between the strange and light quark masses, we determine how this constrains the extrapolation of baryon octet matrix elements and form factors. In particular we can construct certain…

High Energy Physics - Lattice · Physics 2021-12-09 J. M. Bickerton , A. N. Cooke , R. Horsley , Y. Nakamura , H. Perlt , D. Pleiter , P. E. L. Rakow , G. Schierholz , H. Stüben , R. D. Young , J. M. Zanotti

Evidence for the existence of exotic, pentaquark baryons was first found in the invariant mass spectrum of a baryon-meson pair, with the baryon in the octet of flavor SU(3). Exotic pentaquarks may also decay into members of the spin-3/2…

High Energy Physics - Phenomenology · Physics 2007-05-23 Benjamin Grinstein , Mikhail A. Savrov

An explanation of the difference in the values of the apparent $f/d$ ratios for the S- and P- wave amplitudes of nonleptonic hyperon decays is proposed. The argument is formulated in the framework of the standard pole model with…

High Energy Physics - Phenomenology · Physics 2009-10-22 P. Zenczykowski

Treating the strange quark mass as a heavy scale compared to the light quark mass, we perform a matching of the nucleon mass in the SU(3) sector to the two-flavor case in covariant baryon chiral perturbation theory. The validity of the $19$…

Nuclear Theory · Physics 2017-01-31 Xiu-Lei Ren , L. Alvarez-Ruso , Li-Sheng Geng , T. Ledwig , Jie Meng , M. J. Vicente Vacas

In the low-energy regime light and strange baryons should be considered as systems of constituent quarks with confining interaction and a chiral interaction that is mediated by Goldstone bosons as well as by vector and scalar mesons. The…

High Energy Physics - Phenomenology · Physics 2015-06-25 L. Ya. Glozman

By considering a flavour expansion about the SU(3)-flavour symmetric point, we investigate how flavour-blindness constrains octet baryon matrix elements after SU(3) is broken by the mass difference between the strange and light quarks. We…

High Energy Physics - Lattice · Physics 2012-12-12 A. N. Cooke , R. Horsley , Y. Nakamura , D. Pleiter , P. E. L. Rakow , G. Schierholz , J. M. Zanotti

We report an analysis of the impressive new lattice simulation results for octet baryon masses in 2+1-flavor QCD. The analysis is based on a low order expansion about the chiral SU(3) limit in which the symmetry breaking arises from terms…

High Energy Physics - Lattice · Physics 2010-04-06 R. D. Young , A. W. Thomas

We investigate the axial-vector transition form factors of the lowest-lying singly heavy baryons within the framework of the chiral quark-soliton model. We consider the linear $m_{\mathrm{s}}$ corrections, dealing with the strange current…

High Energy Physics - Phenomenology · Physics 2022-12-07 Jung-Min Suh , Hyun-Chul Kim