# Tag Info

15

This is a temperamental difference more than a physical one, but I feel like this question deserves an answer with a lot less formalism than what Urs is using. The physical point that you should never lose sight of is that gauge symmetries are not symmetries at all: they don't map one state to another one, but instead identify a priori different states as ...

11

The mystery here should disappear once one realizes that the BRST complex -- being a dg-algebra -- is the formal dual to a space , namely to the "homotopically reduced" phase space. For ordinary algebras this is more familiar: the algebra of functions $\mathcal{O}(X)$ on some space $X$ is the "formal dual" to $X$, in that maps $f : X \to Y$ correspond to ...

5

Your mechanism of "one ghost falling in" is a different way of talking about the "evaporation of FP ghosts by a black hole". So do black holes evaporate ghosts? This is not a well-defined question because FP ghosts are unphysical, too. They're just a mathematical method to deal with gauge symmetries, in this case the diffeomorphism symmetry. In this sense, ...

5

Why do we gauge-fix the path integral in the first place? If we were doing lattice gauge theory, we didn't need to gauge-fix. But in the continuum case, (the Hessian of) the action for a generalized$^1$ gauge theory has zero-directions that lead to infinite factors when performing the path integral over gauge orbits. In a BRST formulation (such as, e.g., the ...

4

We only have one contribution from each gauge-equivalent matter field configuration: Let $P$ be the principal $G$-bundle associated to our gauge theory on the spacetime $\mathcal{M}$ (for simplicity, assume it is $\mathcal{M} \times G$. The matter fields are constructed as sections of an associated vector bundle $P \times_G V_\rho$, where $V_\rho$ is a ...

4

Here's part of my answer to the derivvation of the EM tensor for the ghost action. It does not match the expression you gave, but I may have made a mistake. CAn you check my work? We start with the action \begin{split} S_{gh} &= - \frac{i}{2\pi} \int d^2 \sigma \sqrt{g} g^{\alpha\mu} b_{\alpha\beta} \nabla_\mu c^\beta \\ \end{split} ...

4

The solution to this problem comes from the sneaky fact (Kugo, 1978) that while the FP ghost field is hermitian $c^\dagger (x) = c(x)$ while the anti-ghost field is anti-hermitian $\bar c^\dagger (x)=-\bar c (x)$ . As a result, the plane wave expansion for the ghost/anti-ghost fields (Becchi, 2008), Scholarpedia are: $$c^a(x)={1 \over(2 \pi)^{3/2}} ... 3 On the torus there are two real moduli \tau_1 and \tau_2, and two conformal Killing vectors corresponding to translations. This means that you need two insertions of b and two insertions of c in order to saturate the zero mode path integral. 3 Most higher derivative theories —and in particular Lee-Wick's model— do not have ghost excitations but they are unstable (Hamiltonian unbounded from bellow). Yes, almost everyone says the opposite but all them are unfortunately wrong. They do not quantize the theory properly. Whenever a degree of freedom has negative energy at the classical level, it must ... 3 As you already wrote, the (3/2)\partial^2 c term is needed for the current to be a one-form i.e. (1,0) tensor field; see also page 131 of Polchinski's String Theory, volume 1. This means that if you compute the OPE$$ T(z) j^{BRST}(0)\sim \dots, $$you want to get$$\dots \sim \frac{1}{z^2} j^{BRST}(0)+\frac{1}{z}\partial j^{BRST}(0), $$see e.g. ... 3 answer for questions 1,2, and 3a 1) Looking at 2.7.22 to 2.7.24 (and also 2.7.18abc), one define the ghost number N^g = \frac{-1}{2\pi i} \int_0^{2 \pi}dz :b(z)c(z): , and that all the operators c_n increase the ghost number by one. [N^g,c_m] = c_m, So the field c(z), made of operators c_m, increase the ghost number by one unit.So ... 3 "Something is conserved for an action" simply means that the action carries a zero overall value of "something" (for an additive quantity). In this case, the action has N_{gh}=0. It follows that the equations of motion derived from the action imply dN_{gh}/dt=0. Most typically, they imply \partial_\mu J^\mu_{gh}=0 i.e. the local continuity law for a ... 3 The central charge counts the number of degrees of freedom only for matter fields living on a flat manifold (or supermanifold in the case of superstrings). An example where this counting argument fails for matter fields is the case of strings moving on a group manifold G whose central charge is given by the Gepner-Witten formula: c = ... 3 The Higgs ghosts are not Faddeev-Popov ghosts. (For starters, the Faddeev-Popov ghosts in the standard model are Grassmann-odd, while the Higgs ghosts are Grassmann-even.) The Higgs ghosts are Goldstone bosons for the spontaneously broken part of the electroweak symmetry SU(2) \times U(1), which, popularly speaking, get eaten by the massive gauge bosons ... 2 Bosonic path integrals :$$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^{-i \large \int ~ dx [\tilde \eta^a \square \eta^a]}$$are not mathematically well-defined, because of the presence of the imaginary unit in the exponential. ... 2 I got it. \epsilon anticommutes with b_A. 2 I did not furnish all the details because it would be too long, but I give some hints at the end of the answer. I have used the formulae :T^g: ~= ~:2(\partial c) b + c(\partial b): and :\frac{1}{2}cT^g: ~= ~:bc \partial c:, when there is an ambiguity in the calculus. We begin by :$$j_B = cT^m+:\frac{1}{2}:cT^g:+\frac{3}{2}\partial^2c=cT^m+:bc\partial ...

2

In a nutshell, the Grassmann-odd Faddeev-Popov ghosts fields appear from the exponentiation of the Faddeev-Popov determinant, i.e., when we write the determinant as a Gaussian integral over Grassmann-odd variables. The Faddeev-Popov determinant can roughly be viewed as a Jacobian factor in the path integral that appears because the path integral variables ...

2

The behaviour of a vector field $v^z$ at $z=\infty$ can be described by first moving to coordinates that are well-defined in that coordinate patch. Defining $w = \frac{1}{z}$, we find $$c^w = \frac{dw}{dz} c^z = - z^{-2} c^z$$ Now, $c^w$ must be well-defined at $w=0$. This implies that $z^{-2} c^z$ must be well-defined as $z \to \infty$. Thus $c^z$ cannot ...

1

I'd say BRST ghosts have more elements of reality compared to longitudinal gauge bosons which are pure gauge. Look at the inner product structure. Physical states belong to the BRST cohomology of BRST-closed modulo BRST-exact. pure gauge longitudinal gauge bosons are BRST-exact and have zero inner product with any other BRST-closed state. BRST ghosts have ...

1

The OP's example is none other than a classic example of Gribov ambiguities. It reflects badly on the choice of BRST formalism more than anything else. It shouldn't be taken to have physical implications.

1

In order to get this term, you have to apply partial integration with respect to one of the coordinates to the action. This leaves you with one integral over two dimensions (with the derivative switched from $c$ to $b$) and an integral over one dimension. If you now vary the second term with respect to $c$ and you acquire Eq. 3.3.28.

1

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 : $\frac{1}{4 \pi}g^{z \bar z}$, Polchinkski write : $\frac{1}{2 \pi}$ So, for instance, the correct expression in $(3.3.24)$ is :  S = \frac{1}{4 \pi} \int d^2z (g^{\bar z z}b_{zz} ...

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