91 \mathrm{nm}$. We can use the energy equation $E = \frac{hc}{\lambda}$, where $h$ is Planck's constant, $c$ is the speed of light, and $\lambda$ is the wavelength. We can then equate this to the Rydberg equation $E = R_H(1 - \frac{1}{n^2})$, where $R_H$ is the
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