Follow the closed question When does the spinor need to be in a grassmann variable?
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Does the spinor in the spinor representation of the space-time symmetry
Lorentz space-time symmetry, like $so(1,d)$ or $spin(1,d)$
Euclidean space-time symmetry, like $so(1+d)$ or $spin(1+d)$
necessarily need to be in a Grassmann variable? So $\psi \eta = -\eta \psi$ for Grassmann variable $\psi$ and $\eta$?