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Related papers: Chiral Multiplets of Large-N Ground State Baryons

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It has recently been suggested that the parity doublet structure seen in the spectrum of highly excited baryons may be due to effective chiral restoration for these states. We argue how the idea of chiral symmetry restoration high in the…

High Energy Physics - Phenomenology · Physics 2009-11-07 T. D. Cohen , L. Ya. Glozman

It is shown that in the large $N_c$ limit the light baryon spectrum exhibits the chiral restoration phase transition at high enough excitation energy. Such a phase transition is evidenced by the systematical parity doublets observed in the…

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

We propose large $N_c$ generalizations for the "diquark" representations of SU(3)$_{\rm flav}$ relevant for positive parity heavy baryons, including putative exotic states. Next, within the framework of the Chiral Quark Soliton Model, we…

High Energy Physics - Phenomenology · Physics 2018-09-26 Michal Praszalowicz

We construct the most general nonlinear representation of chiral SU(2)_L x SU(2)_R broken down spontaneously to the isospin SU(2), on a pair of hadrons of same spin and isospin and opposite parity. We show that any such representation is…

High Energy Physics - Phenomenology · Physics 2009-11-11 Robert L. Jaffe , Dan Pirjol , Antonello Scardicchio

The recent discovery of a narrow resonance in D_s+pi^0 by the BABAR collaboration is consistent with the interpretation of a heavy J^P(0+,1+) spin multiplet. This system is the parity partner of the groundstate (0-,1-) multiplet, which we…

High Energy Physics - Phenomenology · Physics 2008-11-26 William A. Bardeen , Estia J. Eichten , Christopher T. Hill

The algebraic content of chiral symmetry constrains the strong interactions of mesons containing a single heavy quark. We show that the S-wave single-pion transition amplitudes of all heavy meson states are determined as a consequence of…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. R. Beane

In the covariant level-classification scheme of hadrons based on U(12)SF * O(3,1)L symmetry, the ground state baryons and antibaryons are assigned to the (12 * 12 * 12)Sym = 364-multiplet in the spin-flavor U(12)SF symmetry. This multiplet…

High Energy Physics - Phenomenology · Physics 2007-05-23 Muneyuki Ishida , Shin Ishida

The central two-pion exchange NN potential at large distances is studied in the framework of relativistic chiral symmetry and related directly to the nucleon scalar form factor, which describes the mass density of its pion cloud. This…

Nuclear Theory · Physics 2009-11-06 M. R. Robilotta

It has recently been suggested that the parity doublet structure seen in the spectrum of highly excited baryons may be due to effective chiral symmetry restoration for these states. We review the recent developments in this field. We…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. D. Cohen , L. Ya. Glozman

Physics of the low-lying and high-lying hadrons in the light flavors sector is reviewed. While the low-lying hadrons are strongly affected by both $U(1)_A$ and spontaneous $SU(2)_L \times SU(2)_R$ breakings, in the high-lying hadrons these…

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

We demonstrate in a model independent way that, in the combined heavy quark and large N_c limit, there exists a new contracted U(4) symmetry which connects orbitally excited heavy baryons to the ground states.

High Energy Physics - Phenomenology · Physics 2009-10-31 Chi-Keung Chow , Thomas D. Cohen

In the large Nc limit, the mass spectrum of the L=1 orbitally excited baryons N* has a very simple structure, with states degenerate in pairs of spins J=(1/2,3/2), (3/2,5/2), corresponding to irreducible representations (towers) of the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Dan Pirjol , Carlos Schat

The gross features of the observed baryon excitation spectrum below 2 GeV are well explained if the spectrum generating algebra of its intrinsic orbital angular momentum states is o(4)*su(2)_I. The spins of the resonances are obtained…

High Energy Physics - Phenomenology · Physics 2009-10-30 M. Kirchbach

In this paper we investigate the phase structure of a (1+1) and (3+1)-dimensional quark model with four-quark interaction and in the presence of baryon ($\mu_B$), isospin ($\mu_I$) and chiral isospin ($\mu_{I5}$) chemical potentials. It is…

High Energy Physics - Phenomenology · Physics 2018-12-06 T. G. Khunjua , K. G. Klimenko , R. N. Zhokhov-Larionov

The magnetic and transition magnetic moments of the ground-state baryons are computed in heavy baryon chiral perturbation theory in the large-$N_c$ limit, where N_c is the number of colors. SU(3) symmetry breaking is systematically studied…

High Energy Physics - Phenomenology · Physics 2015-03-17 Giovanna Ahuatzin , Ruben Flores-Mendieta , Maria A. Hernandez-Ruiz , Christoph P. Hofmann

We study the evidence for and possible origins of parity doubling among the baryons. First we explore the experimental evidence, finding a significant signal for parity doubling in the non-strange baryons, but little evidence among strange…

High Energy Physics - Phenomenology · Physics 2009-11-11 R. L. Jaffe , D. Pirjol , A. Scardicchio

In this paper we investigate the phase structure of a (1+1)-dimensional schematic quark model with four-quark interaction and in the presence of baryon ($\mu_B$), isospin ($\mu_I$) and chiral isospin ($\mu_{I5}$) chemical potentials. It is…

High Energy Physics - Phenomenology · Physics 2017-01-04 D. Ebert , T. G. Khunjua , K. G. Klimenko

We study the chiral transformation properties of all possible local (non-derivative) interpolating field operators for baryons consisting of three quarks with two flavors, assuming good isospin symmetry. We derive and use the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Keitaro Nagata , Atsushi Hosaka , V. Dmitrašinovi\' c

I discuss the structure of current-induced bottom baryon to charm baryon transitions, and the structure of pion and photon transitions between heavy charm or bottom baryons in the Heavy Quark Symmetry limit as $m_Q\rightarrow\infty$. The…

High Energy Physics - Phenomenology · Physics 2009-10-28 J. G. K"orner

We construct $ {\rm SU(3)}_{\rm L} \otimes {\rm SU(3)}_{\rm R}$ invariant parity doublet models within the linear realization of the chiral symmetry. Describing baryons as the superposition of linear representations should be useful…

High Energy Physics - Phenomenology · Physics 2023-06-28 Takuya Minamikawa , Bikai Gao , Toru kojo , Masayasu Harada
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