SUMMARY
The Jordan-Wigner transform simplifies a spin 1/2 system to a free fermion system in open boundary conditions. However, challenges arise under periodic boundary conditions due to the presence of phase terms, specifically represented by S_N^+S_1^-=(-)^{\sum_{k=1}^{N-1}n_k} a_N^\dagger a_1. This phase term cannot be disregarded, as highlighted in the work of E.H. Lieb, T.D. Schultz, and D.C. Mattis in their 1961 paper. The relationship between periodicity and parity remains a complex issue that requires further exploration.
PREREQUISITES
- Understanding of the Jordan-Wigner transform
- Familiarity with spin 1/2 systems
- Knowledge of free fermion systems
- Basic concepts of periodic boundary conditions in quantum mechanics
NEXT STEPS
- Study the implications of the Jordan-Wigner transform in different boundary conditions
- Examine the paper by E.H. Lieb, T.D. Schultz, and D.C. Mattis for deeper insights
- Research the relationship between periodicity and parity in quantum systems
- Explore advanced topics in fermionic systems and their applications in quantum mechanics
USEFUL FOR
Quantum physicists, researchers in condensed matter physics, and students studying quantum mechanics who are interested in the applications of the Jordan-Wigner transform and boundary conditions.