Calculate $\hbar \ln$ Gaussian Path Integral w/Einstein Summation

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The forum discussion focuses on the calculation of the expression $\hbar \ln \int D x_i \exp[\frac{1}{32 \pi^3} \int ds \int d^3 r x_i(-is,r) M_{ij}(s,r) x_j(is,r)]$ using the Einstein summation convention. The final result is established as $\hbar \int \frac{ds}{2\pi} \ln \det[M_{ij}\delta^3(r-r')]$. Participants discuss the necessity of Fourier transforms and the differences between the variables s and r, with references to the paper by R. Golestanian (2005) for further context. The discussion highlights the importance of understanding the definitions of the variables involved and critiques the original equation presented in the paper.

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MadMax
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Einstein summation convention employed throughout

We want to calculate

\hbar \ln \int D x_i \exp[\frac{1}{32 \pi^3} \int ds \int d^3 r x_i(-is,r) M_{ij}(s,r) x_j(is,r)]

The answer is

\hbar \int \frac{ds}{2\pi} \ln \det[M_{ij}\delta^3(r-r')]

I know that

\int d^3 x_i e^{\frac{1}{2}x_i B_{ij} x_j} = \sqrt{\frac{(2\pi)^n}{\det B_{ij}}}

and that standard logarithmic properties will be used. Also the \delta^3(r-r') means that a Fourier transform involving that delta function will be employed at some point.

Beyond that I'm at a complete loss as to how to continue. One question is why we don't need to employ a Fourier transform involving a \delta(s-s')]. Any help would be much appreciated.
 
Last edited:
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I was hoping someone else would tackle this one, but here goes ...

The answer doesn't make sense to me. I don't see why s should be fundamentally different than r. I think you should have a \delta(s+s'), with + rather than - because the arguments have opposite sign, and that there should be no integral over s.

But perhaps there is something about the definition of x(is,r) that you haven't told us that would change this ...
 
Thanks.

What kind of things might make s different to r in that way?

Perhaps these? "is" is wick rotated frequency; and started out as the Fourier transform of time. r is real space. r is a vector and s is a scalar.
 
Last edited:
MadMax said:
What kind of things might make s different to r in that way?
Perhaps these? "is" is wick rotated frequency; and started out as the Fourier transform of time. r is real space. r is a vector and s is a scalar.

No, none of that should matter.

Is this from a book? If so, which one?
 
He's just being sloppy. His eq.(1) is wrong, and should be what I said. Then he trades log det for Tr log, and the integral over zeta in eq.(3) is part of the trace, just like the integrals over r.
 
Ahh brilliant. Thanks again. :)
 

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