What breaks time reversal symmetry in ferromagnets

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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
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Physicists, particularly those specializing in condensed matter physics, quantum mechanics students, and researchers interested in the properties of ferromagnets and antiferromagnets.

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I am told that in ferromagnets, time reversal symmetry is broken. However, I don't know any hamiltonian terms in solid that can break time reversal symmetry. So is there a hamiltonian term I don't know or is there any subtlety in ferromagnets?
 
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In spontaneous symmetry breaking, there is never a term which explicitly breaks the symmetry in the Hamiltonian
 
OK, I finally learned spontaneous symmetry breaking. However, I am stilled confused. Supposing two local minimum in ferromagnets, time reversal symmetry will transform one into another, both of which are ground states of the Hamiltonian. Thus, it seems that ##T## is actually commutable with ##H##. Then what does time reversal symmetry breaking mean here?
 
T commutes with H, but the ground state is not symmetric under T. That's the general situation in spontaneous symmetry breaking. Likewise, rotational symmetry is also spontaneously broken in a ferromagnet. While the hamiltonian is symmetric under rotations, each of the ground states which are intertransformed under rotations shows a preferred orientation of the spin directions.
 
In fact, the spontaneously broken symmetries cannot be represented as operators in a Hilbert space, as all matrix elements involving two different ground states vanish. That's the formal definition of a spontaneously broken symmetry.
 
DrDu said:
In fact, the spontaneously broken symmetries cannot be represented as operators in a Hilbert space, as all matrix elements involving two different ground states vanish. That's the formal definition of a spontaneously broken symmetry.
I don't understand this. Can you show me an example?
 
The different grounds states belong to what are called different superselection sectors. It means that you basically can't get from one to the other in the thermodynamic limit. If you think of the Ising model, the ordered spin up state and ordered spin down states are degenerate without a magnetic field. However, you cannot get between the two ordered states through spin flips in a finite time in an infinite system.

By the way, the reason that AFs break time reversal is that time reversal flips the spins on each site. AFs also break translation (double the unit cell) but the combination of translation and TR is preserved.
 

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