0000000000400894

AUTHOR

Yasuo Umino

showing 2 related works from this author

Hamiltonian lattice QCD at finite density: equation of state in the strong coupling limit

2001

The equation of state of Hamiltonian lattice QCD at finite density is examined in the strong coupling limit by constructing a solution to the equation of motion corresponding to an effective Hamiltonian describing the ground state of the many body system. This solution exactly diagonalizes the Hamiltonian to second order in field operators for all densities and is used to evaluate the vacuum energy density from which we obtain the equation of state. We find that up to and beyond the chiral symmetry restoration density the pressure of the quark Fermi sea can be negative indicating its mechanical instability. Our result is in qualitative agreement with continuum models and should be verifiabl…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsChiral perturbation theoryNuclear TheoryHigh Energy Physics::LatticeLattice field theoryQCD vacuumAstrophysics (astro-ph)High Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLattice QCDAstrophysicsNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - PhenomenologyHamiltonian lattice gauge theoryHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics - Theory (hep-th)Quantum electrodynamicssymbolsHamiltonian (quantum mechanics)Ground stateLattice model (physics)
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N-quantum approach to quantum field theory at finite T and mu: the NJL model

1999

We extend the N-quantum approach to quantum field theory to finite temperature ($T$) and chemical potential ($\mu$) and apply it to the NJL model. In this approach the Heisenberg fields are expressed using the Haag expansion while temperature and chemical potential are introduced simultaneously through a generalized Bogoliubov transformation. Known mean field results are recovered using only the first term in the Haag expansion. In addition, we find that at finite T and in the broken symmetry phase of the model the mean field approximation can not diagonalize the Hamiltonian. Inclusion of scalar and axial vector diquark channels in the SU(2)$_{rm f}$ $otimes$ SU(3)$_{\rm c}$ version of the …

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryScalar (mathematics)Order (ring theory)FísicaHigh Energy Physics - Phenomenologysymbols.namesakeBogoliubov transformationVacuum energyMean field theorysymbolsQuantum field theoryHamiltonian (quantum mechanics)PseudovectorMathematical physics
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