Since $\phi(t)$ reaches a maximum at $c$, assuming that $\phi''(c)\lt0$, near $c$ we have
$$
\begin{align}
\phi(t)
&=\phi(c)+\phi'(c)(t-c)+\frac12\phi''(t-c)(t-c)^2+O(t-c)^3\\
&=\phi(c)+\frac12\phi''(t-c)(t-c)^2+O(t-c)^3
\end{align}
$$
Thus, $\phi$ behaves like a quadratic function near $c$.
Therefore, we get the stationary phase approximation:
$$
\begin{align}
\int_a^bf(t)e^{x\phi(t)}\,\mathrm{d}t
&\stackrel.=e^{x\phi(c)}\int_a^bf(t)e^{\frac12x\phi''(c)(t-c)^2}\,\mathrm{d}t\\
&\stackrel.=e^{x\phi(c)}f(c)\sqrt{\frac{\vphantom{\lambda}2\pi}{-x\phi''(c)}}
\end{align}
$$