Graduate Integrating Gaussians with complex arguments

Click For Summary
The integral under discussion involves complex arguments and aims to simplify the expression by completing the square. The original integral is transformed into a form that includes a Gaussian integral and an exponential factor, but the user struggles to reproduce the expected result due to the complexity introduced by the conjugate terms. They explore the implications of shifting the variable z, concluding that such a shift does not resolve the issue as it complicates the expression further. The discussion highlights that the method may only work under specific conditions, particularly when J and z are real. Overall, the challenge lies in managing the conjugation and the structure of the integral effectively.
hideelo
Messages
88
Reaction score
15
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)


 
Physics news on Phys.org
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.
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K