Imaginary Partition function

[santale]

I have a partition function in euclidean quantum field theory. I have a parameter, let's say a charge, that I can change in the action that define the partition function.

I found that for small charge the partition function is positive, but there is a critical charge, above the one the partition function becomes negative.

Which is the meaning? Could this be interpreted as a phase transition?

General question: the partition function must be positive? which is the meaning of having an imaginary or negative partition function?

Thanks

 

[andrien]

How can you get a minus sign, the partition function always has the action part exponentiated. Or are you asking something else?

 

[santale]

1) My action has an imaginary current as interaction (due to Wick rotation in from the theory in Minkowski space).
2) From the symmetry if the action I know that the functional integral is positive so the partition function is well defined (it's like the integral of Exp(-x^2+ i x)
3) I want to extimate the partition function through the saddle point method. I find a critical point (that in my case is imaginary) and I expand the theory around it, calculating the second order variation.
4) For small charge, the second order variations are positive, but when I pass a critical charge I find two negative eigenvalues of the second order variation, that gives a factor minus 1 (the negativity of the partition function I refered).

The question is: what does imply the fact that in this case the fact I have a negative contribution? Phase transition? The critical point around the one I was expanding the theory is no more good for large charge?

Thanks

 

[andrien]

You can evaluate the integral in closed form here, it will not be negative. Saddle point method is approximate, also which charge are you talking about? Are you using a scalar field theory with Wick rotation and coupling as charge, then it does not have a critical point.

 

[santale]

The action is Euclidean Yang Mills couled with an heavy static source (this is the imaginary current):
$$F_{\mu\nu}F^{\mu\nu}+i\delta_{\mu0}A_{\mu}$$

Solving the euclidean yang mills equation, I have an imaginary solution.