Time reversal symmetry and Bloch states

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SUMMARY

The discussion focuses on the time reversal symmetry of Bloch states in quantum mechanics. The time reversal operator, denoted as ##\hat{\Theta}##, transforms a Bloch state according to the equation ##\hat{\Theta} \psi_{nk}=\psi^*_{nk}##. It is established that this transformation is valid for scalar functions but not for spinor-valued functions, such as those describing electrons. The discussion concludes that for time reversal invariance, the wavefunctions with momentum k and -k must be energetically degenerate, allowing the formation of invariant wavefunctions like ##\psi_k+\psi_{-k}## and ##i\psi_k-i\psi_{-k}##.

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  • Understanding of quantum mechanics principles, specifically time reversal symmetry
  • Familiarity with Bloch states and their mathematical representation
  • Knowledge of scalar and spinor functions in quantum physics
  • Basic concepts of energy degeneracy in quantum systems
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  • Study the mathematical properties of the time reversal operator in quantum mechanics
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This discussion is beneficial for physicists, particularly those specializing in quantum mechanics, condensed matter physics, and anyone interested in the mathematical foundations of time reversal symmetry and Bloch states.

Joker93
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Hello!

The time reversal operator, ##\hat{\Theta}## transforms a Bloch state as follows:
##\hat{\Theta} \psi_{nk}=\psi^*_{nk}##.
How does one proceed to prove the condition that ##\psi_{nk}## and ##\psi^*_{nk}## must satisfy in order for our system to be time reversal invariant?

Thanks in advance!
 
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First, i would like to point out that your expression is only correct for scalar functions, but not for spinor valued functions, i.e. electrons.
A Bloch function is proportional to exp(ikr) which becomes exp(-ikr) on time reversal. Hence time reversal converts a state with k into one with -k.
In the scalar case, it will be possible to write down an invariant wavefunction if the wavefunctions with k and -k are energetically degenerate. As you then can form ##\psi_k+\psi_{-k}## and ##i\psi_k-i\psi_{-k}##.
 

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