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We calculate the SU(3)-breaking corrections to the hyperon vector coupling $f_1(0)$ up to $\mathcal{O}(p^4)$ in covariant baryon chiral perturbation theory with dynamical octet and decuplet contributions. We find that the decuplet…

High Energy Physics - Phenomenology · Physics 2009-07-30 L. S. Geng , J. Martin Camalich , M. J. Vicente Vacas

The octet and decuplet SU(3)f baryons are studied with the Polyakov, Nambu and Jona-Lasinio model, in a diquark-quark approach, via the resolution of the Bethe-Salpeter equation. This work includes estimations of their masses according to…

High Energy Physics - Phenomenology · Physics 2026-02-10 Eric Blanquier

The charge radii and magnetic moments of all the light and strange baryons are investigated within the framework of a constituent quark model based on Goldstone-boson-exchange dynamics. Following the point-form approach to relativistic…

Nuclear Theory · Physics 2009-11-10 K. Berger , R. F. Wagenbrunn , W. Plessas

We discuss the strong and radiative decays of the decuplet of baryon resonances to the baryon octet in chiral perturbation theory. We comment on the implications for the polarisability of the nucleon.

High Energy Physics - Phenomenology · Physics 2009-10-22 Malcolm Butler , Martin Savage , Roxanne Springer

The covariant spectator formalism is used to model the nucleon and the $\Delta$(1232) as a system of three constituent quarks with their own electromagnetic structure. The definition of the ``fixed-axis'' polarization states for the diquark…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. Ramalho , M. T. Pena , Franz Gross

The role of nonvalence, {\it e.g.} sea quarks and/or meson degrees of freedom in static and quasistatic baryon electroweak observables, is discussed within the phenomenological sum rule approach. The inclusion of nonvalence degrees of…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. B. Gerasimov

We provide a perspective on studies aimed at observing the transition between hadronic and quark-gluonic descriptions of reactions involving light nuclei. We begin by summarizing the results for relatively simple reactions such as the pion…

Nuclear Experiment · Physics 2015-06-05 Roy Holt , R. Gilman

In rare $B$ meson decays $B\rightarrow K \ell^+ \ell^-$, a possible contribution of $\ell^+\ell^-$ emission via photon from the "spectator" quark $q$ ($q=u,d$) in the $B$ meson $(q\bar{b})$ is investigated in addition to the conventional…

High Energy Physics - Phenomenology · Physics 2015-06-16 Hiroyuki Ishida , Yoshio Koide

We present our predictions for meson form factors for the SU(3) octet and investigate their impact on the pion electroproduction cross sections. The electric and magnetic polarizabilities of the SU(3) octet of mesons and baryons are…

High Energy Physics - Phenomenology · Physics 2015-06-17 A. Aleksejevs , S. Barkanova

Magnetic properties of octet baryons are investigated within the framework of chiral perturbation theory. Utilizing a power counting for large magnetic fields, the Landau levels of charged mesons are treated exactly giving rise to baryon…

High Energy Physics - Phenomenology · Physics 2018-01-17 Amol Deshmukh , Brian C. Tiburzi

We present in this talk recent results of the magnetic moments of the baryon antidecuplet within the framework of the chiral quark-soliton model in the chiral limit. The dynamic parameters of the model are fixed by using the experimental…

High Energy Physics - Phenomenology · Physics 2009-11-10 Hyun-Chul Kim , Michał Praszałowicz

A complete and minimal relativistic Lagrangian is constructed at next-to-leading order for SU(3) chiral perturbation theory in the presence of baryon octet and baryon decuplet states. The Lagrangian has 13 terms for the pure decuplet…

High Energy Physics - Phenomenology · Physics 2018-08-01 Måns Holmberg , Stefan Leupold

We calculate the radiative decay widths of decuplet hyperons in a chiral constituent quark model including electromagnetic exchange currents between quarks. Exchange currents contribute significantly to the E2 transition amplitude, while…

Nuclear Theory · Physics 2008-11-26 Georg Wagner , A. J. Buchmann , Amand Faessler

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 analyze the reactions gamma+p => M+B, with M B being either K+ Lambda, K+ Sigma0, or pi+ n, within perturbative QCD, allowing for diquarks as quasi-elementary constituents of baryons. The diquark-model parameters and the quark-diquark…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. Folberth , R. Rossmann , W. Schweiger

We study the magnetic moments of the octet, decuplet, low-lying charm, and low-lying bottom baryons with nonzero light quarks in symmetric nuclear matter using the quark-meson coupling (QMC) model, which satisfies the constraint for the…

High Energy Physics - Phenomenology · Physics 2022-05-04 Kazuo Tsushima

Beyond the spontaneous chiral symmetry breaking scale light and strange baryons should be considered as systems of three constituent quarks with an effective confining interaction and a flavor-spin chiral interaction that is mediated by the…

High Energy Physics - Phenomenology · Physics 2007-05-23 L. Ya. Glozman

We derive covariant wave functions for hadrons composed of two constituents for arbitrary Lorentz boosts. Focussing explicitly on baryons as quark-diquark systems, we reduce their manifestly covariant Bethe-Salpeter equation to covariant…

Nuclear Theory · Physics 2007-05-23 M. Dillig

In this paper the stability of the hedgehog shape of the chiral soliton is studied for the octet baryon with the SU(3) chiral quark soliton model. The strangeness degrees of freedom are treated by a simplified bound-state approach, which…

High Energy Physics - Phenomenology · Physics 2009-11-10 Satoru Akiyama , Yasuhiko Futami

In the present work we calculate the transition magnetic moments for the radiative decays of $\Delta$ baryon to proton $(\Delta \rightarrow p)$ in isospin asymmetric nuclear medium at finite temperature using chiral SU(3) quark mean field…

Nuclear Theory · Physics 2025-04-02 Suneel Dutt , Arvind Kumar , Harleen Dahiya
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