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Related papers: Parity Doubling in the Meson Spectrum

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At zero temperature the negative-parity ground states of the nucleon and delta baryons are non-degenerate with the positive-parity partners due to spontaneous breaking of chiral symmetry. However, chiral symmetry is expected to be restored…

High Energy Physics - Lattice · Physics 2016-10-25 Gert Aarts , Chris Allton , Davide De Boni , Simon Hands , Benjamin Jaeger , Chrisanthi Praki , Jon-Ivar Skullerud

The effect of spontaneous breaking of chiral symmetry over the spectrum of highly excited hadrons is addressed in the framework of a microscopic chiral potential quark model (Generalised Nambu-Jona-Lasinio model) with a vectorial…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yu. S. Kalashnikova , A. V. Nefediev , J. E. F. T. Ribeiro

In this paper, we study the chiral symmetry restoration in the hadronic spectrum in the framework of generalised Nambu-Jona-Lasinio quark models with instantaneous confining quark kernels. We investigate a heavy-light quarkonium and derive…

High Energy Physics - Phenomenology · Physics 2009-11-11 Yu. S. Kalashnikova , A. V. Nefediev , J. E. F. T. Ribeiro

Excited states of $^4$He are studied in four-body calculations with explicitly correlated Gaussian bases. All the levels below $E_{\rm x}$=26 MeV are reproduced reasonably well using realistic potentials. An analysis is made to show how the…

Nuclear Theory · Physics 2008-11-26 W. Horiuchi , Y. Suzuki

Light scalar mesons can be understood as dynamically generated resonances. They arise as 'companion poles' in the propagators of quark-antiquark seed states when accounting for hadronic loop contributions to the self-energies of the latter.…

High Energy Physics - Phenomenology · Physics 2016-08-24 Thomas Wolkanowski

A symmetry-preserving treatment of a vector$\times$vector contact interaction is used to compute spectra of ground-state $J^P = 0^\pm, 1^\pm$ $(f\bar g)$ mesons, their partner diquark correlations, and $J^P=1/2^\pm, 3/2^\pm$ $(fgh)$…

High Energy Physics - Phenomenology · Physics 2021-05-05 Pei-Lin Yin , Zhu-Fang Cui , Craig D. Roberts , Jorge Segovia

The coupled Bethe--Salpeter bound state equations for a $Q\bar Q$ system, where $Q=(U,D)$ is a degenerate, fourth generation, super--heavy quark doublet, are solved in several ladder approximation models. The exchanges of gluon, Higgs and…

High Energy Physics - Phenomenology · Physics 2010-11-01 Pankaj Jain , Alan J. Sommerer , Douglas W. McKay , J. R. Spence , J. P. Vary , Bing--Lin Young

We discuss the mass spectrum of highly-excited nucleon and $\Delta^*$ resonances. The spectrum exhibits parity doublets, pairs of resonances of identical total angular momentum J but of opposite parity. It has been proposed that the parity…

High Energy Physics - Phenomenology · Physics 2009-11-07 Eberhard Klempt

The high-lying mesons in the light quark sector previously obtained from the partial wave analysis of the proton-antiproton annihilation in flight at 1.9 - 2.4 GeV region at CERN reveal a very high degree of degeneracy. This degeneracy can…

High Energy Physics - Phenomenology · Physics 2014-11-20 L. Ya. Glozman , A. Sarantsev

We point out that the spectrum of pseudoscalar and scalar mesons exhibits a cuasi-degenerate chiral nonet in the energy region around 1.4 GeV whose scalar component has a slightly inverted spectrum. Based on the empirical linear rising of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mauro Napsuciale , Simon Rodriguez

In this work we analyse positive- and negative-parity channels for the nucleon (spin $1/2$ octet), $\Delta$ and $\Omega$ baryons (spin $3/2$ decuplet) using lattice QCD. In Nature, at zero temperature, chiral symmetry is spontaneously…

High Energy Physics - Lattice · Physics 2017-04-05 Gert Aarts , Chris Allton , Davide De Boni , Simon Hands , Benjamin Jaeger , Chrisanthi Praki , Jon-Ivar Skullerud

We describe a lattice simulation of the masses and decay constants of the lowest-lying vector and axial resonances, and the electroweak S parameter, in an SU(3) gauge theory with $N_f = 2$ and 6 fermions in the fundamental representation.…

We calculate the low-lying spectra for the positive-parity $\Delta$ and $N$ at two pion masses of 358 and 278 MeV using an isotropic clover action with two degenerate light-quaark and one strange-quark flavors through the application of the…

High Energy Physics - Lattice · Physics 2021-09-30 Tanjib Khan , David Richards , Frank Winter

This work presents a new phenomenological description of QCD vacuum where the color background field is depicted by a constant parallel vector with amplitude proportional to $\sigma\sim 0.28 GeV^2$. The familiar Regge relation can be…

High Energy Physics - Phenomenology · Physics 2008-12-15 Ying Chen

We construct the truly minimal left-right symmetric model by utilizing only the fields dictated by supersymmetry and automatic R-parity conservation. Allowing for non-renormalizable operators in the superpotential, we show that parity can…

High Energy Physics - Phenomenology · Physics 2011-02-09 Charanjit S. Aulakh , Alejandra Melfo , Goran Senjanovic

The global features of spectrum of highly excited light nonstrange mesons can be well understood within both chiral symmetry restoration scenario combined with the relation $M^2\sim J+n$ and within nonrelativistic description based on the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. S. Afonin

We show that if the Standard Model gauge fields and fermions propagate in extra dimenions, a composite Higgs field with the correct quantum number can arise naturally as a bound state due to the strong gauge interactions in higher…

High Energy Physics - Phenomenology · Physics 2009-10-31 Hsin-Chia Cheng

Quark-hadron duality implies that a process described in terms of quark loops should be the hadronic amplitude when averaged over a sufficient number of states. Ambiguities associated with the notion of quark hadron duality can be made…

High Energy Physics - Theory · Physics 2008-11-26 Thomas D. Cohen , Elizabeth S. Werbos

We discuss how the lightest scalars, in particular the broad sigma resonance, can be understood as unitarized (qbar q) states within a unitarized quark model (UQM). The bare (qbar q) scalars are strongly distorted by hadronic mass shifts,…

High Energy Physics - Phenomenology · Physics 2007-05-23 N. A. Tornqvist , A. D. Polosa

Recent studies have completed the A=16 isospin quintets for states with spin/parity J{\pi} =0+ and 2+. The dependence of their masses as a function of isospin projection shows evidence for deviations from quadratic behavior indicating…

Nuclear Theory · Physics 2025-12-15 R. J. Charity , J. Okołowicz , M. Płoszajczak , L. G. Sobotka , K. W. Brown