I encountered the notion of $\mathbb{Z}_2$ symmetry in an article. Can someone give a definition?
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There is an operator $P$ such that $P^2$ is the identity and commutes with the Hamiltonians.
In this case $P=\prod \sigma_x$.
This is a $\mathbb{Z}_2$ because $P$ and the identity form a group isomorphic to the integers modulo 2 (odds and evens)
Identity corresponds to evens, $P$ to odds. $P^2=1$ corresponds to odd plus odd equals even.
If there were some other operators commuting with the Hamiltonians, then would be some other kind of symmetry, not $\mathbb{Z}_2$. But in this case, it is not that complicated.
AHusain
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