The stationary states of a linear potential well are given by the solutions of the following differential equation:
$$\dfrac {\partial^2 f} {\partial x^2} - 2(x - c)f(x) =0$$
On Sakurai's Modern Quantum Mechanics, he claims the substitution $z = 2^{1/3}(x-c)$ transforms this into:
$$\dfrac {\partial^2 f} {\partial z^2} - zf(z) =0$$
Wolfram alpha confirms this solution, but that is not at all evident to me. I would write:
$$\dfrac {\partial^2 f(x)} {\partial z^2} - 2^{1/3}zf(x^2) =0, $$ where $x$ is evaluated at $x = 2^{-1/3}z-c$. I would like to write the equation in the form prescribed by Sakurai, since then the solution is given by Airy's function. What did he do to transform the equation?