simpler katex fix
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				| @ -39,6 +39,17 @@ a & b & c | ||||
| \end{bmatrix} | ||||
| $$ | ||||
| 
 | ||||
| $$ | ||||
| \begin{array}{rll} | ||||
| E \psi &= H\psi & \text{Expanding the Hamiltonian Operator} \\ | ||||
| &= -\frac{\hbar^2}{2m}\frac{\partial^2}{\partial x^2} \psi + \frac{1}{2}m\omega x^2 \psi & \text{Using the ansatz $\psi(x) = e^{-kx^2}f(x)$, hoping to cancel the $x^2$ term} \\ | ||||
| &= -\frac{\hbar^2}{2m} [4k^2x^2f(x)+2(-2kx)f'(x) + f''(x)]e^{-kx^2} + \frac{1}{2}m\omega x^2 f(x)e^{-kx^2} &\text{Removing the $e^{-kx^2}$ term from both sides} \\ | ||||
| & \Downarrow \\ | ||||
| Ef(x) &= -\frac{\hbar^2}{2m} [4k^2x^2f(x)-4kxf'(x) + f''(x)] + \frac{1}{2}m\omega x^2 f(x) & \text{Choosing $k=\frac{im}{2}\sqrt{\frac{\omega}{\hbar}}$ to cancel the $x^2$ term, via $-\frac{\hbar^2}{2m}4k^2=\frac{1}{2}m \omega$} \\ | ||||
| &= -\frac{\hbar^2}{2m} [-4kxf'(x) + f''(x)] \\ | ||||
| \end{array} | ||||
| $$ | ||||
| 
 | ||||
| > [!warn] | ||||
| > Due to limitations in the [underlying parsing library](https://github.com/remarkjs/remark-math), block math in Quartz requires the `$$` delimiters to be on newlines like above. | ||||
| 
 | ||||
|  | ||||
| @ -516,12 +516,5 @@ ol.overflow { | ||||
| 
 | ||||
| .katex-display { | ||||
|   overflow-x: auto; | ||||
|   overflow-y: visible; | ||||
| 
 | ||||
|   & > .katex .katex-html { | ||||
|     .base, | ||||
|     .strut { | ||||
|       display: inline; | ||||
|     } | ||||
|   } | ||||
|   overflow-y: hidden; | ||||
| } | ||||
|  | ||||
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