Evaluating Functional integrals

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Discussion Overview

The discussion centers on the computation of Gaussian functional integrals, particularly in the context of quantum field theory. Participants explore methods for evaluating integrals of the form \( e^{-iS_{0}[\phi]+i(J,\phi)} \) and the implications of different conditions, such as when \( J \) is zero or non-zero.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant inquires about computing Gaussian functional integrals, specifically when \( J \) is non-zero, and expresses confusion regarding the evaluation of functional determinants that depend on \( J(x) \).
  • Another participant suggests that perturbative methods are necessary for evaluation and recommends a specific textbook on quantum field theory.
  • A different participant proposes a technique involving completing the square to simplify the integral, indicating that this method allows for pulling out terms related to \( J^2 \).
  • The initial poster acknowledges the suggestion but raises further questions about evaluating the functional determinant of the operator \( (a\partial^{2} + b)(\phi + J(x)) \).

Areas of Agreement / Disagreement

Participants do not reach a consensus on the methods for evaluating the functional integral and determinant, with multiple approaches and techniques discussed without resolution.

Contextual Notes

Participants express uncertainty regarding the evaluation of functional determinants and the conditions under which finite results can be obtained from the functional integral expressions.

Klaus_Hoffmann
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HOw can you compute a Gaussian functional integral?

i mean integral of the type e^{-iS_{0}[\phi]+i(J,\phi)}

if J=0 then i believe that we can describe the Functional integral as

\frac{c}{(Det(a\partial +b)} a,b,c constant

so Det(a\partial +b)}= exp^{-\zeta '(0)}

\zeta (s) = \sum_{1 \le n}\lambda_{n} ^{-s}

my problem comes when J(x) is different from 0 so we have a functional determinant which is also a function (functional ?? ) of J(x) , then how could yo evaluate it?, also a Fourier transform of a gaussian is again another Gaussian.

Another question..how can you once you have obtained the functional integral Z[J] expressions of the form

\frac{ \delta ^{n}Z[J]}{ \delta J(x1) \delta J(x2)...}

so you get finite results ??
 
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You can't except perturbatively. The perturbation expansion is explained in any good book on QFT, try Zee's QFT in a Nutshell for example.
 
Sorry I see I misread, the trick is to complete the square. You add J^2 - J^2 write the whole thing as (phi + J)^2 and pull the J^2 term out of the integral.
 
thank you everybody.. f-h hit the correct answer (thankx) however still we have the problem that how could you evaluate the functional Determinant.

Det( a\partial ^{2} +b) of the operator:

( a\partial ^{2} +b)(\phi +J(x))
 

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