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Related papers: Exploring a new SU(4) symmetry of meson interpolat…

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Recently, a new symmetry of mesons has been found upon truncation of the quasi-zero modes of the Overlap Dirac operator in lattice simulations. Namely, the $\rho,\rho',\omega,\omega',a_1, b_1,h_1$ and possibly $f_1$ $J=1$ mesons get…

High Energy Physics - Lattice · Physics 2015-05-14 M. Denissenya , L. Ya. Glozman , M. Pak

Recently a global SU(4) \supset SU(2)_L \times SU(2)_R \times U(1)_A symmetry of the confining Coulombic part of the QCD Hamiltonian has been discovered with N_F=2. This global symmetry includes both independent rotations of the left- and…

High Energy Physics - Phenomenology · Physics 2016-05-26 L. Ya. Glozman

Recently a large degeneracy of $J=1$ mesons, that is larger than the $SU(2)_L \times SU(2)_R \times U(1)_A$ symmetry of the QCD Lagrangian, has been discovered upon truncation of the near-zero modes from the valence quark propagators. It…

High Energy Physics - Lattice · Physics 2015-11-04 M. Denissenya , L. Ya. Glozman , M. Pak

In this talk we first overview lattice results that have led to the observation of new SU(2)_{CS} and SU(2N_F) symmetries upon artificial truncation of the near-zero modes of the Dirac operator at zero temperature and at high temperature…

High Energy Physics - Lattice · Physics 2018-08-29 L. Ya. Glozman

Recent lattice results on Dirac low-mode removed $J=1,2$ mesons and $J=\frac{1}{2}$ baryons reveal the appearance of a new $SU(4)$ symmetry of confinement. Here the degeneracy of all $J=2$ iso-vector states within an irreducible…

High Energy Physics - Lattice · Physics 2015-11-02 M. Denissenya , L. Glozman , M. Pak

The classical part of the QCD partition function (the integrand) has, ignoring irrelevant exact zero modes of the Dirac operator, a local SU(2N_F) \supset SU(N_F)_L \times SU(N_F)_R \times U(1)_A symmetry which is absent at the Lagrangian…

High Energy Physics - Lattice · Physics 2018-02-14 L. Ya. Glozman

The correlation function of meson interpolators in $N_f=2+1+1$ lattice QCD with optimal domain-wall quarks at the physical point are studied for six temperatures in the range $ T \sim$ 190-770 MeV. The meson interpolators include a complete…

High Energy Physics - Lattice · Physics 2023-06-06 Ting-Wai Chiu

A large degeneracy of mesons of a given spin has recently been discovered upon reduction of the quasi-zero modes of the Dirac operator in a dynamical lattice simulation. Here a symmetry group that is responsible for this degeneracy is…

High Energy Physics - Phenomenology · Physics 2015-06-22 L. Ya. Glozman

Using the chirally invariant overlap Dirac operator we remove its lowest-lying quasizero modes from the valence quark propagators and study evolution of isovector mesons with J=1. At the truncation level about 50 MeV SU(2)_L \times SU(2)_R…

High Energy Physics - Lattice · Physics 2014-06-10 M. Denissenya , L. Ya. Glozman , C. B. Lang

In a local gauge-invariant theory with massless Dirac fermions a symmetry of the Lorentz-invariant fermion charge is larger than a symmetry of the Lagrangian as a whole. While the Dirac Lagrangian exhibits only a chiral symmetry, the…

High Energy Physics - Phenomenology · Physics 2019-01-14 L. Ya. Glozman

We study the isoscalar and isovector $J=0,1$ mesons with the overlap operator within two flavour lattice QCD. After subtraction of the lowest-lying Dirac eigenmodes from the valence quark propagator all disconnected contributions vanish and…

High Energy Physics - Lattice · Physics 2015-04-16 M. Denissenya , L. Ya. Glozman , C. B. Lang

We construct an explicit example of dimensional reduction of the free massless Dirac operator with an internal SU(3) symmetry, defined on a twelve-dimensional manifold that is the total space of a principal SU(3)-bundle over a…

High Energy Physics - Theory · Physics 2015-06-26 Petko A. Nikolov , Gergana R. Ruseva

In a dynamical lattice simulation with the overlap Dirac operator and $N_f=2$ mass degenerate quarks we study all possible $J=0$ and $J=1$ correlators upon exclusion of the low lying "quasi-zero" modes from the valence quark propagators.…

High Energy Physics - Lattice · Physics 2015-05-25 M. Denissenya , L. Ya. Glozman , C. B. Lang

While the QCD Lagrangian as the whole is only chirally symmetric, its electric part has larger chiral-spin SU(2)_{CS} and SU(2N_F) symmetries. This allows separation of the electric and magnetic interactions in a given reference frame.…

High Energy Physics - Phenomenology · Physics 2020-11-11 L. Ya. Glozman

We have applied a new gauge-invariant, noncompact, Monte Carlo method to simulate the $U(1)$, $SU(2)$, and $SU(3)$ gauge theories on $8^4$ and $12^4$ lattices. The Creutz ratios of the Wilson loops agree with the exact results for $U(1)$…

High Energy Physics - Lattice · Physics 2009-10-28 Kevin Cahill , Gary Herling

We show that nuclear interactions are SU(4) symmetric at leading order in chiral perturbation theory in the large-N limit of QCD. The nucleons and delta resonances form a 20-dimensional representation of SU(4) and we show how Wigner's…

High Energy Physics - Phenomenology · Physics 2019-08-15 David B. Kaplan , Martin J. Savage

Enlarged symmetry characterized by the group SU(4) can be realized in isolated semiconducting quantum dots. A Hubbard model then describes a pillar array of coupled dots and at half-filling the system can be mapped onto an SU(4) spin chain.…

Mesoscale and Nanoscale Physics · Physics 2008-02-03 Alexey Onufriev , Brad Marston

We study the SU(3)-invariant relevant deformation of D=4 N=4 SU(N) gauge theory at large N using the AdS/CFT correspondence. At low energies, we obtain a nonsupersymmetric gauge theory with three left-handed quarks in the adjoint of SU(N).…

High Energy Physics - Theory · Physics 2014-11-18 Jacques Distler , Frederic Zamora

We investigate the spatial $ z $-correlators of meson operators in $ N_f=2+1+1+1 $ lattice QCD with optimal domain-wall quarks across eight temperatures ranging from 325 to 3250 MeV. The meson operators include a complete set of Dirac…

High Energy Physics - Lattice · Physics 2025-05-07 Ting-Wai Chiu

Vertex symmetry for interacting fermions will be shown to lead to a Lagrangian exhibiting $SU(2N)_W$ invariance associated with the subgroup $SU(2N)_q \times SU(2N)_{\bar{q}}$ generated by $C$-odd and $C$-even spin operators. Approximate…

High Energy Physics - Theory · Physics 2007-05-23 Sultan Catto
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