# Partition function for bosons with path integral

In this book the partition function for bosons is defined in eq. 2.17 as:

$$Z=\mathrm{Tr}[e^{-\beta (H-\mu_i N_i)}]=\sum_a\int d\phi_a\langle\phi_a|e^{-\beta(H-\mu_i N_i)}|\phi_a\rangle$$ The following two points are not really clear to me:

1. Why do I need the integral $$\int d\phi_a$$? To evaluate a trace I usually only need the sum over some complete set of states?

2. What is the meaning of the $$\phi_a$$'s? Right now I imagine them as a complete set, i.e. I can decompose every function as

$$\phi(\vec{x})=\sum_aw_a\phi_a(\vec{x})$$

where $$w_a$$ are some coeficients.

A general state

$$\hat{\phi}(\vec{x},0)|\phi\rangle=\phi(\vec{x})|\phi\rangle$$

is a decomposition:

$$|\phi\rangle=\sum_a w_a|\phi_a\rangle$$

• Minor comment to the post (v3): Please consider to mention explicitly author, title, etc. of link, so it is possible to reconstruct link in case of link rot. Mar 21, 2022 at 5:47

In the first expression (judging purely on the basis of the formal expression), the index $$a$$ would normally represent some internal degree of freedom such as spin. In that case, it is not an index of a discrete set of functions. A path integral involves a continuous set of functions ("paths"). Therefore you would need the functional integration over all these functions in addition to the summation over the spins.

The result of your expressions would then only be valid in the case where you have a discrete set of orthogonal functions and the index would label all these functions. That would not be the case for your first expression.

However, there is a way that people represent functional integrals so that they come closer to ordinary integrals. This approach seems to be what the text in the linked book does. The assumption is that the elements of functional space can be expanded in terms of some orthonormal basis of functions $$\psi(\mathbf{x}) = \sum_n \phi_n \Phi_n(\mathbf{x}) .$$ Here $$\Phi_n(\mathbf{x})$$ represents an element of a discrete (countable) infinite set of functions and $$\phi_n$$ denotes the coefficients. The functional integration measure is then represented as $$\mathcal{D}[\psi] = \Pi_n \text{d} \phi_n .$$ In other words, a functional integral would be represented by $$\int W[\psi] \mathcal{D}[\psi] = \int W(\phi_n) \Pi_n \text{d} \phi_n .$$ So the integral runs over all the (infinite number of) coefficients.

To evaluate a trace in this context, we need to assume that there are complete sets of states associated with each element of the basis. In other words, if we pick $$\Phi_n(\mathbf{x})$$ with a specific $$n$$, then we have a complete orthogonal basis $$|\phi_n\rangle$$ associated with this chosen function. The different values of the associated coefficient parameterizes the respective elements of this basis. Since the coefficient vary continuously, the associated basis must also be a continuous basis. The trace is now evaluated by performing the overlap of the functional with all the elements of all these bases. For each basis, we need to integrate over the coefficient that labels the elements of the continuous basis. Then we also need to sum over all the different basis. Therefore, such a trace takes the form of the OP's first expression.

• I don't think that this is true. Have a look at section 2.6 in the book
– user255856
Mar 18, 2022 at 16:34
• In the book eq. (2.103) contains a product and not a summation. Is that a typo in your first expression? Mar 19, 2022 at 3:23
• My first eq. is just eq. 2.17 in the book. Hmm yeah it might be a typo. But I am very sceptical that the authors would make such an essential typo is a book...
– user255856
Mar 20, 2022 at 3:23
• Also why should the trace involve a product? The sum actually makes sense...
– user255856
Mar 20, 2022 at 3:24
• See my edited answer Mar 23, 2022 at 3:56

For general non-interacting bosonic fields(which is often the very starting point of each story, like perturbation theory), their diagonalized Hamiltonian in $$\mathbf{k}$$ space is $$\hat{H}_{0}=\sum_{\mathbf{k}} \omega_{\mathbf{k}} \hat{b}_{\mathbf{k}}^{\dagger} \hat{b}_{\mathbf{k}}$$ For every single mode we can define its coherent state as before $$\hat{b}_{\mathbf{k}}|\phi_{k}\rangle=\phi_{k}|\phi_{k}\rangle$$.

So basically I think the index $$\alpha$$ in your problem accounts for different modes.

And of course, as @flippiefanus mentioned, when spin degrees or other internal degrees are involved, the index $$\alpha$$ also has to run through them. But one has to note that for scalar bosons there is no spin, which is a huge difference from fermions.

You can find more information in chapter 5 of this book: Kamenev, A. (2011). Field Theory of Non-Equilibrium Systems. Cambridge: Cambridge University Press. doi:10.1017/CBO9781139003667 and hopefully you can verify or correct my statements then.