3D two-color QCD at finite temperature and baryon density
arXiv:hep-ph/0306220 · doi:10.1016/j.nuclphysb.2003.07.024
Abstract
We study the phase diagram for two-color QCD in three-dimensional spacetime, as a function of temperature and baryon chemical potential, using the low-energy effective Lagrangian approach. We show one-loop renormalizability at zero temperature, and then use the one-loop effective Lagrangian at finite temperature and chemical potential to show that at low temperature there is a critical line separating the normal and diquark phase, with this critical line ending at a tricritical point. This phase structure is qualitatively similar to that found recently by Splittorff et al for two-color QCD in four-dimensional spacetime, although the details are quite different, due to the different symmetries and the different loop and infrared properties of three-dimensional spacetime.
14 pp, 1 fig
References in corpus (4)
Cited by in corpus (14)
- Quark-meson-diquark model for two-color QCD
- The QCD Sign Problem for Small Chemical Potential
- Thermal pion masses in the second phase:
- Phase transitions and gluodynamics in 2-colour matter at high density
- Diquark and Pion Condensation in Random Matrix Models for two-color QCD
- Effect of short-range interactions on the quantum critical behavior of spinless fermions on the honeycomb lattice
- QCD in One Dimension at Nonzero Chemical Potential
- Phase Diagram of the Dirac Spectrum at Nonzero Chemical Potential
- Fluctuation-induced higher-derivative couplings and infrared dynamics of the Quark-Meson-Diquark Model
- Review of Vector Condensation at High Chemical Potential
- Universality crossover between chiral random matrix ensembles and twisted SU(2) lattice Dirac spectra
- Anomalous superfluidity in 2+1 dimensional two-color lattice QCD
- Chiral dynamics and pion properties at finite temperature and isospin chemical potential
- Chiral limit of 2-color QCD at strong couplings