Peskin & Schroeder p. 285, change of variables integration measure

naele
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I had a question about about the integration measure for the path integral after a unitary change of variables. First they consider a 4D spacetime lattice with volume L^4. The measure is
<br /> \mathcal{D}\phi = \prod_i d\phi(x_i)<br />

They expand the field variables in a Fourier series \phi(x_i)=\frac{1}{V}\sum_n e^{-ik_n\cdot x_i}\phi(k_n). My questions are as follows:
1) Why do they consider the real and imaginary parts of \phi(k_n) as independent variables?
2) Why do they re-write the measure as
<br /> \mathcal{D}\phi(x)=\prod_{k_n^0&gt;0}dRe\phi(k_n)dIm \phi(k_n)<br />

I've never seen a measure re-written like that, I was wondering what allows them to do so.

There's already a thread about this here but I wasn't comfortable bumping a three year old thread, and the response didn't clear up my confusion.

I appreciate any help.
 
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Bear in mind that this is a functional measure. That means that what they're trying to do is consider every possible value that \phi(k) could take on at position k_i. Since the Fourier transform requires \phi to be complex, we need a way to parameterize all of the complex plane. We can do this by defining \phi in terms of two real numbers a and b, by setting \phi(k) = a(k) + i b(k), and integrating both of them over the entire real line, leading to an integration measure of da\:db. Writing d Re\phi\:d Im\phi is just another way of saying the same thing.
 
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I think I understand that part now, thanks. I do have a problem still with the change of variables from \phi(x_i)\to\phi(k_n). I might be missing something, but there would presumably be a factor of V^{1/n} from the 1/V factor in the Fourier series expansion. And then when I transform from \phi(k_n)\phi^*(k_n)\to Re \phi(k_n)Im \phi(k_n) I get a Jacobian that's not equal to 1.
 
For your first question, I think the answer is that we're just dealing with the measure, not the full integral. So the 1/V will probably show up in the full integral expression.

As for the Jacobian of the measure, that one may have been my fault--I think you need to define the parameterization as \phi = \frac{a + ib}{\sqrt{2}} or something like that in order for the Jacobian to work out correctly.
 
Well the reason I thought there would be a factor is because, unless I'm doing something wrong, I thought the jacobian for \phi(x_i)\to\phi(k_n) is \frac{1}{V}e^{-ik_n\cdot x_i}. Although now that I think about it, they do say that it is a unitary transformation, so presumably the Jacobian would have unit modulus, but I'm having difficulties checking that.
 
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