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We treat baryons as bound states of scalar or axialvector diquarks and a constituent quark which interact through quark exchange. We obtain fully four-dimensional wave functions for both octet and decuplet baryons as solutions of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. Alkofer , S. Ahlig , C. Fischer , M. Oettel , H. Reinhardt

The contributions from the $qqqq\bar q$ components to the magnetic moments of the octet as well as the $\Delta^{++}$ and $\Omega^-$ decuplet baryons are calculated for the configurations that are expected to have the lowest energy if the…

Nuclear Theory · Physics 2014-11-18 C. S. an , Q. B. Li , D. O. Riska , B. S. Zou

The magnetic polarisabilities of octet baryons are calculated close to the physical quark-mass point using the background field method in lattice QCD. This first calculation draws on the identification and elimination of exceptional…

High Energy Physics - Lattice · Physics 2024-12-13 Thomas Kabelitz , Waseem Kamleh , Derek Leinweber

The chiral quark model suggests that the baryon quark-sea is negatively polarized. This modifies the spin structure as given by the naive quark model and agrees with experimental data. However, for the magnetic moments, there is significant…

High Energy Physics - Phenomenology · Physics 2009-10-30 T. P. Cheng , Ling-Fong Li

In this work, the electromagnetic and gravitational form factors of $\Delta$ isobars, as well as the electromagnetic $N-\Delta$ transition form factors are studied systematically and continuously using a covariant quark-diquark approach…

High Energy Physics - Phenomenology · Physics 2026-02-24 Jiaqi Wang , Dongyan Fu , Yubing Dong

With the chiral quark model, we have calculated the axial charges of the pentaquark states with $(I,I_3)=(\frac{1}{2},\frac{1}{2})$ and $J^{P}=\frac{1}{2}^{\pm},\frac{3}{2}^{\pm},\frac{5}{2}^{\pm}$. The $P_c$ states with the same $J^P$…

High Energy Physics - Phenomenology · Physics 2017-01-04 Guang-Juan Wang , Zhan-Wei Liu , Shi-Lin Zhu

The strange magnetic form factor of the nucleon is studied in the heavy baryon chiral effective approach at next to leading order. The one loop contributions from kaon and intermediate octet and decuplet hyperons are included, using…

High Energy Physics - Phenomenology · Physics 2015-06-18 P. Wang , D. B. Leinweber , A. W. Thomas

A symmetry-preserving Dyson-Schwinger equation treatment of a vector-vector contact interaction is used to compute dressed-quark-core contributions to the nucleon $\sigma$-term and tensor charges. The latter enable one to directly determine…

Nuclear Theory · Physics 2015-04-08 Mario Pitschmann , Chien-Yeah Seng , Craig D. Roberts , Sebastian M. Schmidt

We propose an ultimate upgrade of the Karl- Sehgal (KS) formula which relates baryon magnetic moments to the spin structure of constituent quarks, by adding anomalous magnetic moments of quarks. We first argue that relativistic nature of…

High Energy Physics - Phenomenology · Physics 2011-09-08 M. Mekhfi

We calculate the intensities and angular distributions of positive and negative muons produced by atmospheric neutrinos. We comment on some sources of uncertainty in the charge ratio. We also draw attention to a potentially interesting…

Astrophysics · Physics 2011-05-12 T. K. Gaisser , Todor Stanev

An operator formalism is used on the wavefunction of baryons to compute their charge radii and quadrupole moments. Total anti-symmetric wavefunction in spin, color and flavor space is framed for $J^P=\frac{1}{2}^+$ nucleons and…

High Energy Physics - Phenomenology · Physics 2023-10-04 Preeti Bhall , Meenakshi Batra , Alka Upadhyay

The effective strange quark and antiquark masses are estimated from the chiral soliton approach (CSA) results for the spectrum of exotic and nonexotic baryons. There are problems when one tries to project results of the CSA on the simple…

High Energy Physics - Phenomenology · Physics 2013-09-11 Vladimir B. Kopeliovich

The recent unbiased measurements of the electric form factor of the neutron suggest that its shape may be interpreted as a smooth broad distribution with a bump at Q^2 \approx 0.3(GeV/c)^2 superimposed. As a consequence the corresponding…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. Friedrich , Th. Walcher

The baryonic form factor of charged pions is studied in detail in the Nambu--Jona-Lasinio model with constituent quarks, where the spontaneously broken chiral symmetry is the key dynamical ingredient guaranteeing the would-be Goldstone…

High Energy Physics - Phenomenology · Physics 2022-08-17 Wojciech Broniowski , Enrique Ruiz Arriola , Pablo Sanchez-Puertas

The proton and neutron electromagnetic form factors and the nucleon axial form factor have been calculated in the Goldstone-boson exchange constituent-quark model within the point-form approach to relativistic quantum mechanics. The…

High Energy Physics - Phenomenology · Physics 2017-08-23 S. Boffi , M. Radici , L. Glozman , R. F. Wagenbrunn , W. Plessas , W. Klink

We report an analysis of the octet baryon masses using the covariant baryon chiral perturbation theory up to next-to-next-to-next-to-leading order with and without the virtual decuplet contributions. Particular attention is paid to the…

Nuclear Theory · Physics 2017-08-23 Xiu-Lei Ren , Li-Sheng Geng , Jie Meng

New results on baryon structure and spectrum developed in collaboration with Dan Riska [1-4] are reported. The main idea is that beyond the chiral symmetry spontaneous breaking scale light and strange baryons should be considered as systems…

High Energy Physics - Phenomenology · Physics 2014-11-17 L. Ya. Glozman

There is evidence that the properties of hadrons are modified in a nuclear medium. Information about the medium modifications of the internal structure of hadrons is fundamental for the study of dense nuclear matter and high-energy…

Nuclear Theory · Physics 2025-05-09 G. Ramalho , K. Tsushima , Myung-Ki Cheoun

The electromagnetic form factors of the spin-3/2 $\Omega$ baryons, namely $\Omega$, $\Omega_c^\ast$, $\Omega_{cc}^\ast$ and $\Omega_{ccc}$, are calculated in full QCD on $32^3\times 64$ PACS-CS lattices with a pion mass of 156(9) MeV. The…

High Energy Physics - Lattice · Physics 2016-01-06 K. U. Can , G. Erkol , M. Oka , T. T. Takahashi

We calculate baryon decuplet to octet electromagnetic transition form factors in quenched and partially quenched chiral perturbation theory. We work in the isospin limit of SU(3) flavor, up to next-to-leading order in the chiral expansion,…

High Energy Physics - Lattice · Physics 2009-11-10 Daniel Arndt , Brian C. Tiburzi
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