Solving Schrodinger for harmonic oscillator(griffiths analytic method)

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I was just getting into quantum mechanics. But I'm having a bit of trouble following Griffiths for the analytic method. It goes like so:

The Schrodinger equation is:

$$-\frac{\hbar^2}{2m}\frac{d^2\psi}{d x^2} + \frac{1}{2} m \omega^2 x^2 \psi = E \psi $$

Griffiths expresses $\xi$ as:

$$\xi = \sqrt{\frac{m \omega}{\hbar}}x$$

and $K$ as:

$$K=\frac{2E}{\hbar \omega}$$

Ultimately, leading to the equation:

$$\frac{d^2\psi}{d\xi^2}=(\xi^2-K) \psi$$

I've tried to rearrange on my own, but:

  1. I do not understand why $\xi$ equals the square root, except for $x$. $\xi$ is eventually squared.