# Evaluate the Propagator for particle going around a circle

I'm new to path integrals

I want to show that $$\langle x_1|e^{-\beta H}|x_2\rangle\ = \ Z_0\sum_{n=-\infty}^{\infty}exp\bigg(-\frac{m}{2\beta \hbar}[(x_2-x_1) \ + \ nL)]^2\bigg)$$ (where $\beta = k_BT , H=-\frac{\hbar^2}{2m}\frac{d^2}{dx^2}$, and $Z_0$ is the diagonal matrix element $\langle x|e^{-\beta H}|x\rangle$ for a free particle) for a particle moving in a circle length $L$ such that paths may wind a number n times around it, and the path $x(\tau)$ for $0<\tau<\beta \hbar$ satisfies the boundary conditions $x(0)=x_1, x(\beta \hbar)=x_2$, by writing $$x(\tau) = x_1\ + \frac{\tau}{\beta \hbar}[(x_2-x_1) \ + \ nL)]^2\ +\ s(\tau),$$ where $s(\tau)$ satisfies the boundary condition $s(0)=0$, $s(\beta \hbar)=0$ and does not wrap around the circle.

The Euclidean action when evaluated is

$$S[x(\tau)] = \frac{m}{2\beta \hbar}[(x_2-x_1) \ + \ nL)]^2 \ +\ \int_{0}^{\beta \hbar}d\tau\frac{m}{2}\bigg(\frac{ds}{d\tau}\bigg)^2$$

My first thought is to just use the propagator formula

$$\langle x_1|e^{-\beta H}|x_2\rangle\ = N\int Dx(\tau)e^{-\frac{1}{\hbar}S[x(\tau)]}$$

but with imaginary time $\tau=it$ from $0$ to $\beta$.

I think the second term of S should seperate out as $Z_0$ with N but i'm not sure how it is the diagonal element, is it because of the boundary conditions of s(t) as that represents going from x to x? and I'm not sure how you can just turn the other part of the integral into a sum?

full question - http://www-thphys.physics.ox.ac.uk/courses/C6/C6web2012/PS1.pdf q6c

• Extremely closely related: The position-representation matrix elements of the propagator for a particle in a ring. That propagator is one hairy beast for real times, but at least you're using it at imaginary times where the series does converge. What, exactly, do you want to know about that propagator? Aug 31, 2017 at 22:31
• I'm just not sure how to get from the integral form of the propagator to the sum form, I think I understand how to get $Z_0$ but not the sum part Sep 1, 2017 at 11:20
• Yeah, I'm not that sure how to handle the path integral there. The Schulman references in the linked question treat it in significant detail, though, as I recall. Sep 1, 2017 at 13:35

As far as I can tell, you have two questions. I will answer them separately. Throughout I will set $\hbar = 1$.

1) Where does the sum $\sum_{n = -\infty}^{\infty}$ come from?

The standard path integral form for the propagator of a free particle is

$$\langle x_{2} | e^{-\beta H} | x_{1} \rangle = \int \mathcal{D} x(\tau) \exp(-S_{E}[x(\tau)]),$$

where the integrals runs over all paths $x(\tau)$ satisfying the boundary conditions $x(0) = x_{1}$ and $x(\beta)=x_{2}$, and $S_{E}$ is the Euclidean action.

The crux of this answer relies on the fact that in the path integral, we integrate over all possible paths satisfying the given boundary conditions. What the change of variables from $x(\tau)$ to $s(\tau)$ does is to make how we count these paths more explicit.

In the question we define a variable $s(\tau)$ that satisfies $s(0) = s(\beta) = 0$. Other than these boundary conditions, $s(\tau)$ is completely unrestricted (i.e. it is not restricted to a circular topology). Now, for each choice of $s(\tau)$, we can define a path

$$x_{n}(\tau) = x_{1} + \dfrac{\tau}{\beta} \left[(x_{2}-x_{1}) + n L \right] + s(\tau),$$

for some integer $n$, and this will be a valid path for the path integral, since the circular topology means that we identify points modulo $L$. Furthermore, between the choices for $s(\tau)$ and $n$, we have enumerated all possible paths that satisfy the given boundary conditions.

Thus, in the expression for the propagator, we have to integrate over $s(\tau)$ and sum over $n$ to make sure we account for all possible paths $x(\tau)$. This gives us the expression

$$\langle x_{2} | e^{-\beta H} | x_{1} \rangle = \sum_{n} \int \mathcal{D} s(\tau) \exp(-S_{E}[x_{n}(\tau)]),$$

with $x_{n}(\tau)$ given as above.

2) Why should $Z_{0}$ be the diagonal matrix element of the propagator on $\mathbb{R}$?

As you stated in your question, the Euclidean action $S_{E}[x_{n}(\tau)]$ separates into two parts, given by

$$S_{E}[x_{n}(\tau)] = S_{n} + S_{E}[s(\tau)],$$

where $S_{n} = \frac{m}{2 \beta} \left[ (x_{2} - x_{1}) + n L \right]^{2}$. This separation is helpful because it separates the dependence on $n$ and $s(\tau)$.

Since $S_{n}$ is a constant, we can factor it out of the path integral. This part gives the summand in the expression for the propagator that you are trying to derive.

The remaining part is

$$\int \mathcal{D} s(\tau) \exp(-S_{E}[s(\tau)]),$$

where we recall that the path $s(\tau)$ has the boundary conditions $s(0) = s(\beta) = 0$, but is otherwise unrestricted (i.e. it is not restricted to a circular topology). But this is precisely what we'd write for the propagator of a free particle in one dimension moving from $x=0$ to $x=0$ in imaginary time $\beta$! And from translational invariance, this shouldn't depend on the fact that the particle starts and finishes at $x=0$, just the fact that the path is periodic. Hence the remaining part gives us $Z_{0} = \langle x | e^{-\beta H} | x \rangle$ for a free particle moving on the real line. This is the "diagonal" matrix element of the propagator because it is simply the propagator $\langle x_{2} | e^{-\beta H} | x_{1} \rangle$ evaluated at $x_{1} = x_{2} = x$.

I am on mobile, so will not be able to give equations, will be very hand wavy. In case you need more explanation I will elaborate. For spaces of non trivial topologies like the case asked here, to get to proper continuum path integral representation you need to use resolution of identities conforming to the state space under consideration i.e., avoiding double counting. Further you will have to use for this case poisson summation formula. You can find very good discussion about it in Kleinert's or Schulman's books.