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The light scalar meson spectrum is studied using the improved ladder QCD with the UA(1) breaking Kobayashi-Maskawa-'t Hooft interaction by solving the Schwinger-Dyson and Bethe-Salpeter equations. The dynamically generated…

High Energy Physics - Phenomenology · Physics 2009-11-10 Toru Umekawa , Kenichi Naito , Makoto Oka , Makoto Takizawa

The mass spectra of singly charmed and bottom baryons, $\Lambda_{c/b}(1/2^\pm,3/2^-)$ and $\Xi_{c/b}(1/2^\pm,3/2^-)$, are investigated using a nonrelativistic potential model with a heavy quark and a light diquark. The masses of the scalar…

High Energy Physics - Phenomenology · Physics 2020-07-15 Yonghee Kim , Emiko Hiyama , Makoto Oka , Kei Suzuki

We present the current status of the MILC collaboration's calculations of the properties of the light pseudoscalar meson sector. We use asqtad staggered ensembles with 2+1 dynamical flavors down to $a \approx 0.045$ fm and light quark mass…

In this paper, the possibility to have new physics is considered at the scale of the electroweak symmetry breaking (EWSB) in a completely new framework. A new non-standard minimal chiral fermion extension of the Standard Model (SM) which…

High Energy Physics - Phenomenology · Physics 2015-09-15 D. A. Camargo

We give a survey of recent development and applications of the chiral quark soliton model (also called the Nambu-Jona-Lasinio soliton model) with $N_f$=2 and $N_f$=3 quark flavors for the structure of baryons. The model is an effective…

High Energy Physics - Phenomenology · Physics 2009-10-30 Teruaki Watabe , Klaus Goeke

Recent theoretical developments of hadrons in nuclei are briefly reviewed in the aspect of chiral symmetry in nuclei. We show a general sum rule connecting in-medium hadronic quantities and quark condensate, emphasizing that both pionic…

Nuclear Theory · Physics 2010-12-17 Daisuke Jido

Most of the exotic hidden-charm hadrons discovered over the last 20 years fit neatly into the quark model as normal mesons and baryons if the existence of a seventh flavor of quark is hypothesized. For the quark to reproduce the spectrum…

High Energy Physics - Phenomenology · Physics 2026-03-31 Scott Chapman

Among the newly observed structures in the heavy quarkonium mass region, some are proposed to be hadronic molecules. We investigate the consequences of heavy quark flavor symmetry on these heavy meson hadronic molecules. The symmetry allows…

High Energy Physics - Phenomenology · Physics 2013-09-19 Feng-Kun Guo , Carlos Hidalgo-Duque , Juan Nieves , Manuel Pavon Valderrama

The so-called extended linear sigma model is a chiral model with (pseudo)scalar and (axial-)vector mesons. It is based on the requirements of (global) chiral symmetry and dilatation invariance. The purpose of this model is the description…

High Energy Physics - Phenomenology · Physics 2017-08-23 F. Giacosa , D. Parganlija , P. Kovacs , Gy. Wolf

We report on our recent progress in the generation of resonant behavior in unitarized meson-meson scattering amplitudes obtained from Chiral Perturbation Theory. These amplitudes provide simultaneously a remarkable description of the…

High Energy Physics - Phenomenology · Physics 2009-11-10 J. R. Pelaez , A. Gomez Nicola

We review recent studies of light scalar meson properties by means of unitarization techniques, obtained from dispersion theory, and applied to the Chiral Perturbation Theory expansion. In particular, light scalars do not follow the N_c…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. R. Peláez , G. Ríos

The approximate chiral invariance of the two-flavor QCD is known to be spontaneously broken. This effect explains the relatively small pion mass and, as is widely believed, the mass splittings of would-be chiral partners --- the hadrons of…

High Energy Physics - Phenomenology · Physics 2014-10-09 S. S. Afonin

The masses of baryons containing a single heavy quark are studied in a combined expansion in $1/m_Q$, $1/N_c$ and $SU(3)$ flavor symmetry breaking. Heavy quark baryon mass splittings are related to mass splittings of the octet and decuplet…

High Energy Physics - Phenomenology · Physics 2008-11-26 Elizabeth Jenkins

By means of unitarized Chiral Perturbation Theory it is possible to obtain a remarkable description of meson-meson scattering amplitudes up to 1.2 GeV, and generate poles associated to scalar and vector resonances. Since Chiral Perturbation…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. R. Pelaez

After commenting on the state of contemporary hadronic physics and spectroscopy, I highlight four areas where the action is: searching for the relevant degrees of freedom, mesons with beauty and charm, chiral symmetry and the D_{sJ} levels,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chris Quigg

A new selection rule is described for the vector mesons in the decuplet representations of flavor SU(3)

High Energy Physics - Phenomenology · Physics 2009-11-10 S. U. Chung , E. Klempt

Assuming the spin-independence for confining force, we give a covariant quark representation of general composite meson systems with definite Lorentz transformation properties. For benefit of this representation we are able to deduce…

High Energy Physics - Phenomenology · Physics 2009-10-31 Shin Ishida , Muneyuki Ishida , Tomohito Maeda

Theoretical predictions are given for the light-flavor sea-quark distributions including the strange quark ones on the basis of the flavor SU(3) version of the chiral quark soliton model. Careful account is taken here of the SU(3) symmetry…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. Wakamatsu

Using the chiral soliton model and heavy quark symmetry we study baryons containing two heavy quarks. If there exists a stable (under strong interactions) meson consisting of two heavy quarks and two light ones, then we find that there…

High Energy Physics - Phenomenology · Physics 2009-12-30 Myron Bander , Anand Subbaraman

We enlarge the chiral model, the so-called extended Linear Sigma Model (eLSM), by including the low-lying hybrid nonet with exotic quantum numbers $J^{PC}=1^{-+}$ and the nonet of their chiral partners with $J^{PC}=1^{+-}$ to a global…

High Energy Physics - Phenomenology · Physics 2022-04-18 Walaa I. Eshraim
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