How do you find the asymptotic expansion of $\int_{-\infty}^{\infty} e^{ix\left(\frac{t^3}{3}+t\right)}dt $ as $x \to \infty$ ?
I know that I will eventually have to use the fact that $\int_{-\infty}^{\infty} e^{-xt^2}dt = \frac{\sqrt{\pi}}{\sqrt{x}}$ but not sure how to get to this point.
Any hints/help would be appreciated!
Let $f(x)$ denote the integral. Substituting $t = 2\sinh\left(\frac{1}{3}\operatorname{arsinh}z\right)$, the integral reduces to
\begin{align*} f(x) &= \frac{2}{3}\int_{-\infty}^{\infty}\exp\left(\frac{2xi}{3}z\right)\cosh\left(\frac{1}{3}\operatorname{arsinh}z\right) \frac{1}{\sqrt{1+z^2}} \, \mathrm{d}z \end{align*}
Noting that the integrand is $\mathcal{O}\bigl( e^{-\frac{2x}{3}\operatorname{Im}(z)} |z|^{-2/3} \bigr)$ as $|z| \to \infty$ with $\operatorname{Im}(z)>0$, we can deform the contour to a Hankel-type contour wrapping around the principal branch cut $[i,i\infty)$ of the integrand. The resulting integral is
\begin{align*} f(x) &= \frac{2}{3}\int_{i+0^+}^{i\infty+0^+}\exp\left(\frac{2xi}{3}z\right)\cosh\left(\frac{1}{3}\operatorname{arsinh}z\right) \frac{1}{\sqrt{1+z^2}} \, \mathrm{d}z \\ &\quad - \frac{2}{3}\int_{i-0^+}^{i\infty-0^+}\exp\left(\frac{2xi}{3}z\right)\cosh\left(\frac{1}{3}\operatorname{arsinh}z\right) \frac{1}{\sqrt{1+z^2}} \, \mathrm{d}z. \end{align*}
Substituting $z = it \pm 0^+$ to each of the integral, respectively,
\begin{align*} f(x) &= \frac{2}{3}\int_{1}^{\infty} \exp\left(-\frac{2x}{3}t\right)\cosh\left(\frac{i\pi}{6} + \frac{1}{3} \operatorname{arcosh}t\right) \frac{1}{\sqrt{t^2-1}} \, \mathrm{d}t \\ &\quad + \frac{2}{3}\int_{1}^{\infty} \exp\left(-\frac{2x}{3}t\right)\cosh\left(\frac{i\pi}{6} - \frac{1}{3} \operatorname{arcosh}t\right) \frac{1}{\sqrt{t^2-1}} \, \mathrm{d}t \\ &= \frac{2}{\sqrt{3}}\int_{1}^{\infty} \exp\left(-\frac{2x}{3}t\right)\cosh\left(\frac{1}{3} \operatorname{arcosh}t\right) \frac{1}{\sqrt{t^2-1}} \, \mathrm{d}t \\ &= \frac{1}{\sqrt{3}}\int_{-\infty}^{\infty} \exp\left(-\frac{2x}{3}\cosh s\right)\cosh\left(\frac{1}{3}s\right) \, \mathrm{d}s. \tag{$t=\cosh s$} \end{align*}
The asymptotic behavior of the last integral as $x \to \infty$ can be studied using Laplace's method, yielding
$$ f(x) \sim e^{-2x/3} \sqrt{\frac{\pi}{x}} \quad \text{as } x \to \infty. $$