This exercise may be solved by means of the Fourier cosine series expansion
$$ f(e^{i\theta})=\sum_{n=0}^\infty a_n \cos(n\theta),$$
with $\displaystyle a_n=\dfrac{\int_{0}^{2\pi} \overline{f(e^{i\theta})}\cos(n\theta)d\theta}{\int_{0}^{2\pi} \cos^2(n\theta)d\theta}$.
Here we recall that for $z=e^{i\theta}$, we have $z^n+\frac{1}{z^n}=2\cos(n\theta)$ ($n \in \mathbb{Z}$).
Thus, using the fact that $\cosh(z+\frac{1}{z})=\cosh(2\cos(\theta))$ and $$\int_{0}^{2\pi} \cos^2(n\theta)d\theta=\pi$$ we realize that
$\displaystyle a_n=\frac{1}{2\pi}\int_{0}^{2\pi} 2\cos(n\theta)\cosh(2\cos(\theta))d\theta.$ (essentially the same to be proved but written in polar coordinates).
A good exercise (to get in touch with the complex analysis formalism) is to show that the coefficients $a_n$ computed above may be rewritten as a Cauchy integral formula over the unit disk $|z|=1$, involving the $n-$derivative of $f(z)=\cosh(z+\frac{1}{z})$.