The linear sigma model at a finite isospin chemical potential
arXiv:hep-ph/0606241 · doi:10.1088/0954-3899/32/11/012
Abstract
The effect of finite isospin chemical potential to the effective masses of the mesons at finite temperature is investigated in the framework of the O(4) linear sigma model with explicit chiral symmetry breaking. We present a mechanism to include the isospin chemical potential in the model. By using the Cornwall-Jackiw-Tomboulis method of composite operators, we obtain a set gap equations for the effective masses of the mesons and get the numerical results in the Hartree approximation. We find that the introduction of the chemical potential only affects the mass of the charged pions and sigma, while there is almost NO effects on the mass of neutral pions.
11 pages, 6 figures; Version to appear in J. Phys. G
References in corpus (19)
- QCD at finite isospin density
- Static and Dynamic Critical Phenomena at a Second Order QCD Phase Transition
- The Quark-Gluon Plasma in Equilibrium
- QCD-like Theories at Finite Baryon Density
- Emergence of Coherent Long Wavelength Oscillations After a Quench: Application to QCD
- On two-color QCD with baryon chemical potential
- Pion Superfluidity and Meson Properties at Finite Isospin Density
- Chiral Symmetry Restoration at Nonzero Temperature in the SU(3) \times SU(3) Linear Sigma Model
- Self-consistent Improvement of the Finite Temperature Effective Potential
- A calculation of the QCD phase diagram at finite temperature, and baryon and isospin chemical potentials
- Thermalization at RHIC
- The O(N) Model at Finite Temperature: Renormalization of the Gap Equations in Hartree and Large-N Approximation
- Thermal Pions at Finite Isospin Chemical Potential
- Chiral symmetry restoration in linear sigma models with different numbers of quark flavors
- Linear sigma model and chiral symmetry at finite temperature
- Thermal Effective Potential of the O(N) Linear sigma Model
- Effective Potential of O(N) Linear Sigma Model at Finite Temperature
- Thermal pion masses in the second phase:
- Bose-Einstein condensation and chiral phase transition in linear sigma model
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- Thermodynamics and susceptibilities of isospin imbalanced QCD matter
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- Functional Renormalization for Chiral and U_A(1) Symmetries at Finite Temperature
- Topological Susceptibility in Three-Flavor Quark Meson Model at Finite Temperature
- Probing the hadron mass spectrum in dense two-color QCD with the linear sigma model
- Stressed Cooper pairing in QCD at high isospin density: effective Lagrangian and random matrix theory
- On the symmetry improved CJT formalism in the linear sigma model
- Pionic BEC--BCS crossover at finite isospin chemical potential
- Pion condensation in the two--flavor chiral quark model at finite baryochemical potential
- Magnetic Corrections to - Scattering Lengths in the Linear Sigma Model
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- Linear Sigma Model at Finite Temperature and Baryonic Chemical Potential Using the Midpoint Technique