SUMMARY
The Wigner-Mermin theorem establishes that continuous symmetry breaking cannot occur in two-dimensional systems with short-range interactions at finite temperatures, which implies that spontaneous positional order and magnetization are absent in such systems. This theorem does not rule out other types of phase transitions, such as Kosterlitz-Thouless transitions, which are relevant for vortices. Additionally, non-equilibrium two-dimensional systems can exhibit phase transitions, as evidenced by polariton Bose-Einstein condensates (BECs). The discussion highlights the relevance of the Bose-Hubbard model in understanding SF-Mott transitions, with significant literature available, including the influential paper by Fisher.
PREREQUISITES
- Understanding of the Wigner-Mermin theorem
- Familiarity with SF-Mott insulator transitions
- Knowledge of Kosterlitz-Thouless transitions
- Basic concepts of Bose-Hubbard models
NEXT STEPS
- Research the implications of the Wigner-Mermin theorem on phase transitions
- Study the Bose-Hubbard model in detail
- Explore Kosterlitz-Thouless transitions and their significance in two-dimensional systems
- Investigate experimental realizations of Mott transitions, particularly in polariton BECs
USEFUL FOR
Physicists, researchers in condensed matter physics, and students studying phase transitions and quantum systems will benefit from this discussion.