Discovering Z Symmetry: Understanding its Role in Physics

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Hi all,

Have anyone heard about a symmetry called " Z symmetry " . It's considered a discrete symmetry, in which terms at a Lagrangian for example can take "Z charges" 0, 1 or +1 to be invariant or non-invariant under this symmetry ..

I heard about before, but I try to find any reference for it. I found only rotational groups like ##Z_2## and ##Z_4##.


S.
 
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what about it?
 
I need a reference about ,
also I don't remember exactly, when we give "Z charges " for the fields in a term like say : ## d^c e^+ \phi ##, when
this term is invariant or not invariant under this symmetry.
 
if you try to do a discrete symmetry, in front of your terms you will have:
(-1)^{\sum_i Q_i}
invariant is when it's plus (so you have the same result)
not invariant if it's minus (because you got a minus in front).
It's pretty similar to a U(1) symmetry, because a broken U(1) gives you the Z2.

Now I guess, if you have a Z_N group, looking at it as the Nth root of unity, then in order to be invariant it has to belong to the identity again...
 
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