The asymptotics of the generalised Bessel function

We demonstrate how the asymptotics for large $|z|$ of the generalised Bessel function $${}_0\Psi_1(z)=\sum_{n=0}^\infty\frac{z^n}{\Gamma(an+b) n!},$$ where $a>-1$ and $b$ is any number (real or complex), may be obtained by exploiting the well-established asymptotic theory of the generalised Wright function ${}_p\Psi_q(z)$. A summary of this theory is given and an algorithm for determining the coefficients in the associated exponential expansions is discussed in an appendix. We pay particular attention to the case $a=-1/2$, where the expansion for $z\to\pm\infty$ consists of an exponentially small contribution that undergoes a Stokes phenomenon. We also examine the different nature of the asymptotic expansions as a function of $\arg\,z$ when $-1<a<0$, taking into account the Stokes phenomenon that occurs on the rays $\arg\,z=0$ and $\arg\,z=\pm\pi(1+a)$ for the associated function ${}_1\Psi_0(z)$. These regions are more precise than those given by Wright in his 1940 paper. Numerical computations are carried to verify several of the expansions developed in the paper.