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lsdragon
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Fermionic Parity operator or number operator are not conserved after Bogoliubov transformation
In fact, the relations that you given to preserve anti-commutation relation is equivalent to have an unitary $M$. You can directly check it by multiplication and using the relations you derived.
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Fermionic Parity operator or number operator are not conserved after Bogoliubov transformation
The fermionic parity operator should be preserved by a Bogoliubov transformation, right?
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Why chiral Majorana fermions with finite momentum are called as an Majorana fermion?
So people call $\gamma(p)$ a Majorana fermion because $\gamma(x) = \int dp e^{ip x} \gamma(p)$ is a Majorana fermion. So is there an original paper mention it ? Just curious about it.
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