Integrating Gaussians with complex arguments

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Discussion Overview

The discussion revolves around the integration of a complex Gaussian function of the form \(\int_\mathbb{C} dz \: \exp\left(-\frac{1}{2}K|z|^2 + \bar{J}z\right)\), where \(K\) is a real constant and \(J\) is a complex constant. Participants are exploring the implications of completing the square in this integral and the challenges that arise due to the nature of complex conjugation.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant expresses difficulty reproducing a result from a textbook, suggesting that the term \(|z|^2\) complicates the completion of the square due to its dependence on conjugation.
  • Another participant proposes that a shift in the variable \(z\) could simplify the integral, specifically suggesting \(z' = z - \frac{2J}{K^2}\).
  • A different participant counters that shifting \(z\) does not resolve the issue, arguing that it introduces additional terms that complicate the expression and prevent the integral from being factored as desired.
  • Another participant notes that the method may only work if both \(J\) and \(z\) are real numbers, indicating a potential limitation in the approach.
  • One participant suggests that if the original exponent included an additional term \(+J\bar{z}\), it might lead to a successful integration.

Areas of Agreement / Disagreement

Participants do not appear to reach consensus on the method for integrating the complex Gaussian function. Multiple competing views and approaches are presented, with some participants expressing skepticism about the effectiveness of shifting \(z\) and others suggesting alternative modifications.

Contextual Notes

The discussion highlights limitations related to the assumptions about the nature of \(J\) and \(z\), as well as the dependence on the specific form of the exponent in the integral. There are unresolved mathematical steps and conditions that affect the validity of the proposed approaches.

hideelo
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The integral I'm looking at is of the form

\int_\mathbb{C} dz \: \exp \left( -\frac{1}{2}K|z|^2 + \bar{J}z \right)

Where K \in \mathbb{R} and J \in \mathbb{C}

The book I am following (Kardar's Statistical Physics of Fields, Chapter 3 Problem 1) asserts that by completing the square this becomes Z \exp\left( \frac{- |J|^2}{2K} \right) where Z = \int_\mathbb{C} dz \: \exp \left( -\frac{1}{2}K|z|^2 \right). I can't seem to reproduce this, and I think the trouble I'm running into arises from |z|^2 not being a square, but rather it involves conjugation as well. Therefore, I get the following

-\frac{1}{2}K|z|^2 + \bar{J}z = -\frac{1}{2}K\left( z\bar{z} -2 \frac{\bar{J}}{K}z \right)= -\frac{1}{2}K\left( z\bar{z} -2 \frac{\bar{J}}{K}z - 2 \frac{J}{K}\bar{z} +2 \frac{J}{K}\bar{z} + 4\frac{ |J|^2}{K^2} - 4 \frac{ |J|^2}{K^2} \right) =

-\frac{1}{2}K\left( z - 2 \frac{J}{K} \right) \left( \bar{z} -2 \frac{\bar{J}}{K} \right) -J\bar{z} +2 \frac{ |J|^2}{K}

Which means that I'm getting that

\int_\mathbb{C} dz \: \exp \left( -\frac{1}{2}K|z|^2 + \bar{J}z \right) = \left[ \int_\mathbb{C} dz \: \exp \left( -\frac{1}{2}K \left| z-2 \frac{J}{K} \right|^2 - J\bar{z} \right) \right] \exp\left( 2 \frac{ |J|^2}{K} \right)

Which doesn't at all seem like

\left[ \int_\mathbb{C} dz \: \exp \left( -\frac{1}{2}K|z|^2 \right) \right] \exp\left( \frac{- |J|^2}{2K} \right)


 
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I haven't worked through all the details, but it looks like there was a shift in ##z##, i.e. ##z'=z-\frac{2J}{K^2}##.
 
mathman said:
I haven't worked through all the details, but it looks like there was a shift in ##z##, i.e. ##z'=z-\frac{2J}{K^2}##.

I don't think shifting z by anything can help. Suppose you sent z \mapsto z+a for any a then I would get the following

-\frac{1}{2}K |z|^2+\bar{J}z \mapsto -\frac{1}{2}K |z+a|^2+\bar{J}(z + a) =
-\frac{1}{2}K \left( z\bar{z} + a\bar{z} + z\bar{a} +a\bar{a} -\frac{2\bar{J}}{K} z - \frac{2\bar{J}}{K}a \right) =
-\frac{1}{2}K \left( z\bar{z} + a\bar{z} + z \left( \bar{a} - \frac{2\bar{J}}{K} \right) +a\bar{a} - \frac{2\bar{J}}{K}a \right)

If I want this to look like -\frac{1}{2}K|z+b|^2 + c, then I need to add and subtract terms with \bar{z} which means that I can't pull e^c out of the integral.
 
I'm getting a similar problem. It looks it will work only if ##J## and ##z## are real.
 
If the original exponent had an additional term ##+J\bar z##, it might work.
 

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