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In article <[EMAIL PROTECTED]>, "Squark" <[EMAIL PROTECTED]> wrote: > "Aaron Bergman" <[EMAIL PROTECTED]> wrote in message > news:[EMAIL PROTECTED] > > Let's say you're doing a path integral over some bosons and fermions. > > The fermion path integral ends up being a Pfaffian of some operator on > > bosonic fields. However, the Pfaffian is not usually a function on the > > space of bosonic fields (reduced by gauge equivalence for gauge theories > > or just in general for something like sigma model anomalies), rather it > > is a section of a line bundle. > > How come? Are you saying exp(iS_fermionic) take values in a line bundle? Not quite. The path integral over the fermions gives something that's a section of a line bundle. Why is it a line bundle? Because it's a Pfaffian. The Pfaffian is the squar root of the determinant. There's necessarily a choice of sign there. As usual, locally this is easy, but globally you get a line bundle, not necessarily trivial. > Also, does it mean one cannot have gauge anomalies without fermions? Yes. Aaron
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