We simulate two-flavour lattice QCD with at a finite chemical potential ~1 for isospin, and finite temperature. At small ,u~, we determine the position of the crossover from hadronic matter to a quark-gluon plasma as a function of ~1. At larger ~1 we observe the phase transition from the superfluid
Lattice QCD at finite isospin chemical potential and temperature
β Scribed by J.B. Kogut; D.K. Sinclair
- Publisher
- Elsevier Science
- Year
- 2003
- Tongue
- English
- Weight
- 251 KB
- Volume
- 119
- Category
- Article
- ISSN
- 0920-5632
No coin nor oath required. For personal study only.
β¦ Synopsis
We simulate lattice QCD at a finite chemical potential ~1 for isospin (1s) at zero and finite temperatures. At some ~1 = pc QCD has a second order transition with mean-field critical exponents to a state where ( 13) is broken spontaneously by a charged pion condensate. Heating the system with PI > /I~ we find there is some temperature at which this condensate evaporates. This transition appears to be second order and mean-field at lower ~1 values, and first order for ~1 sufficiently large. We are determining the dependence of the finite temperature crossover T, on ~11 for ~1 < pc. This is expected to be identical to Tc's dependence on quark-number chemical potential ~1~ for small ~1~.
π SIMILAR VOLUMES