Integrating Gaussians with complex arguments

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SUMMARY

The integral discussed 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 "Statistical Physics of Fields" by Kardar claims that completing the square leads to Z \exp\left(\frac{-|J|^2}{2K}\right), with Z = \int_\mathbb{C} dz \: \exp\left(-\frac{1}{2}K|z|^2\right). The user struggles to reproduce this result due to the complexity of |z|^2 involving conjugation, leading to an alternative expression that does not match the expected outcome. The discussion highlights the challenges of manipulating complex variables in integrals.

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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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