We study the effects of Lorentz non-invariance on the physical pion velocity at the critical temperature $T_c$ in an effective theory of hidden local symmetry (HLS) with the "vector manifestation" fixed point. We match at a "matching scale" $\Lambda_M$ the axial-vector current correlator in the HLS with the one in the operator product expansion for QCD, and present the matching condition to determine the bare pion velocity. We find that the physical pion velocity, which is found to be one at $T=T_c$ when starting from the Lorentz invariant bare HLS, remains close to one with the Lorentz non-invariance, $v_\pi (T_c) = 0.83 - 0.99$. This result is quite similar to the pion velocity in dense matter
In vacuum, in the chiral limit the coupling of a pion to two on-shell photons is directly related to...
For an exact chiral symmetry which is spontaneously broken at zero temperature, we show that at nonz...
: The width of the process ß 0 ! flfl is calculated within effective QCD at finite temperature. We...
We study the pion velocity near the critical temperature $T_c$ of chiral symmetry restoration in QCD...
We study the pion velocity at the critical temperature of chiral symmetry restoration in QCD. Starti...
Based on talks given at "Chiral 02," Kyoto, Japan, 7-9 October 2002 and "SCGT02," Nagoya, Japan, 10-...
Lecture given at 2002 International Workshop on ``Strong coupling Gauge Theories and Effective Field...
We define a family of non local and chirally symmetric low energy lagrangians motivated by theoretic...
In this write-up, I summarize the recent development of the hidden local symmetry (HLS) theory as an...
Recent developments in our description of RHIC and related heavy-ion phenomena in terms of hidden lo...
We review the relationship between the pion decay constant $f_\pi$, the chiral symmetry restoration ...
26 pages, 4 eps figsWe analyze a pion form factor formulation which fulfills the Analyticity require...
We investigate the shear viscosity of a pion gas in relativistic kinetic theory, using the Nambu-Jon...
We have developed a field theory formalism to calculate in-medium properties of hadrons within a uni...
We extend an effective Lagrangian embodying broken scale and chiral symmetry to include explicit chi...
In vacuum, in the chiral limit the coupling of a pion to two on-shell photons is directly related to...
For an exact chiral symmetry which is spontaneously broken at zero temperature, we show that at nonz...
: The width of the process ß 0 ! flfl is calculated within effective QCD at finite temperature. We...
We study the pion velocity near the critical temperature $T_c$ of chiral symmetry restoration in QCD...
We study the pion velocity at the critical temperature of chiral symmetry restoration in QCD. Starti...
Based on talks given at "Chiral 02," Kyoto, Japan, 7-9 October 2002 and "SCGT02," Nagoya, Japan, 10-...
Lecture given at 2002 International Workshop on ``Strong coupling Gauge Theories and Effective Field...
We define a family of non local and chirally symmetric low energy lagrangians motivated by theoretic...
In this write-up, I summarize the recent development of the hidden local symmetry (HLS) theory as an...
Recent developments in our description of RHIC and related heavy-ion phenomena in terms of hidden lo...
We review the relationship between the pion decay constant $f_\pi$, the chiral symmetry restoration ...
26 pages, 4 eps figsWe analyze a pion form factor formulation which fulfills the Analyticity require...
We investigate the shear viscosity of a pion gas in relativistic kinetic theory, using the Nambu-Jon...
We have developed a field theory formalism to calculate in-medium properties of hadrons within a uni...
We extend an effective Lagrangian embodying broken scale and chiral symmetry to include explicit chi...
In vacuum, in the chiral limit the coupling of a pion to two on-shell photons is directly related to...
For an exact chiral symmetry which is spontaneously broken at zero temperature, we show that at nonz...
: The width of the process ß 0 ! flfl is calculated within effective QCD at finite temperature. We...