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Ghosts are unphysical states that arise when quantizing gauge theories. Do not use this tag for 'ghosts' in the paranormal sense.

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A question about surface term of ghost fields

Partial answer : I think that the problem, in Polchinski book, is that the terms $g^{z \bar z} (=2)$, are systematically non explicitely written, that is, instead of : $\frac{1}{4 \pi}g^{z \bar z}$ …
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5 votes
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How do I show the existence of a conserved ghost number with BRST in bosonic string theory?

answer for questions $1$,$2$, and $3a$ 1) Looking at $2.7.22$ to $2.7.24$ (and also $2.7.18abc$), one define the ghost number $N^g = \frac{-1}{2\pi i} \int_0^{2 \pi}dz :b(z)c(z):$ , and that all the …
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4 votes
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A question about BRST current in bosonic string theory

I did not furnish all the details because it would be too long, but I give some hints at the end of the answer. I have used the formulae $:T^g: ~= ~:2(\partial c) b + c(\partial b):$ and $:\frac{1}{2 …
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3 votes

How to get the $i\epsilon$ prescription for a Faddeev-Popov ghost propagator?

Bosonic path integrals : $$Z = \int D\phi ~e^{-i \large \int ~ dx [\frac{1}{2}\phi (\square+m^2)\phi]}$$ or Femionic path integrals (like Fadeev-Popov ghosts) : $$Z = \int D\eta D \tilde \eta ~e^{- …
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