Assuming that
[tex]U(t,x)=\int_{-\infty}^\infty F(x,\tau)e^{it\tau}\,d\tau[/tex]
we come to
[tex]-ib\frac{\partial^2 F(x,\tau)}{\partial x^2}-iax\frac{\partial F(x,\tau)}{\partial x}+\tau F(x,\tau)=0[/tex]
which solution is as follows
[tex]F(x,\tau) = x[H1(\tau)KummerM(-\frac{-2a+i\tau}{2a},\frac{3}{2},\frac{ax^2}{2b})+H2(\tau)KummerU(-\frac{-2a+i\tau}{2a},\frac{3}{2},\frac{ax^2}{2b})]e^{-\frac{ax^2}{2b}}[/tex]
so the general solution to your PDE is
[tex]U(t,x)=xe^{-\frac{ax^2}{2b}}\int_{-\infty}^\infty [H1(\tau)KummerM(-\frac{-2a+i\tau}{2a},\frac{3}{2},\frac{ax^2}{2b})+H2(\tau)KummerU(-\frac{-2a+i\tau}{2a},\frac{3}{2},\frac{ax^2}{2b})]e^{it\tau}\,d\tau[/tex]
where H1 and H2 are arbitrary functions.