SUMMARY
In ferromagnets, time reversal symmetry is broken due to spontaneous symmetry breaking, despite the Hamiltonian being symmetric under time reversal. The ground states of a ferromagnet, while intertransformable under time reversal, exhibit a preferred orientation of spin directions, leading to the conclusion that time reversal symmetry is not represented as an operator in the Hilbert space. The Ising model exemplifies this phenomenon, where ordered spin states are degenerate but cannot transition between each other in a thermodynamic limit. Additionally, antiferromagnets (AFs) break time reversal symmetry by flipping spins on each site, although the combination of translation and time reversal remains preserved.
PREREQUISITES
- Understanding of Hamiltonian mechanics in quantum physics
- Familiarity with spontaneous symmetry breaking concepts
- Knowledge of the Ising model in statistical mechanics
- Basic principles of ferromagnetism and antiferromagnetism
NEXT STEPS
- Study the implications of spontaneous symmetry breaking in quantum systems
- Explore the Ising model and its applications in ferromagnetism
- Investigate the role of superselection sectors in quantum mechanics
- Learn about the relationship between symmetry and ground states in condensed matter physics
USEFUL FOR
Physicists, particularly those specializing in condensed matter physics, quantum mechanics students, and researchers interested in the properties of ferromagnets and antiferromagnets.