Step 1: Relate ionization to the energy of the incident radiation.
Ionization of a hydrogen atom in its ground state ($n=1$) means exciting the electron from $n=1$ to $n=\infty$ (free electron).
The minimum energy required for this process is the ionization energy ($E_{ion}$).
The energy of the incident radiation must be equal to or greater than $E_{ion}$.
Step 2: Find the ionization energy for the hydrogen atom.
The energy of an electron in the $n^{th}$ orbit of a hydrogen atom is $E_n = -\frac{13.6}{n^2} \text{ eV}$.
The ground state energy ($n=1$) is $E_1 = -13.6 \text{ eV}$.
The energy of the ionized state ($n=\infty$) is $E_\infty = 0 \text{ eV}$.
\[
E_{ion} = E_\infty - E_1 = 0 - (-13.6 \text{ eV}) = 13.6 \text{ eV}.
\]
Step 3: Relate the energy to the maximum wavelength.
The energy of a photon is $E = \frac{hc}{\lambda}$. For the maximum wavelength ($\lambda_{max}$), the energy must be minimum and equal to $E_{ion}$.
\[
\lambda_{max} = \frac{hc}{E_{ion}}.
\]
Step 4: Use the shortcut formula for $\lambda_{max$.}
The product $hc$ is often given in electron-volt meters: $hc \approx 1240 \text{ eV}\cdot\text{nm}$ or $12400 \text{ eV}\cdot\text{\AA}$.
We use the $\text{\AA}$ version since the options are in $\text{\AA}$.
\[
\lambda_{max} = \frac{12400 \text{ eV}\cdot\text{\AA}}{13.6 \text{ eV}}.
\]
\[
\lambda_{max} \approx 911.76 \text{ \AA}.
\]
Step 5: Conclude the result.
The maximum wavelength is nearly $912 \text{ \AA}$.