Concept:
The wavelength ($\lambda$) of a photon emitted during an electronic transition in a hydrogen-like atom or ion is given by the Rydberg formula:
$$\frac{1}{\lambda} = R Z^2 \left(\frac{1}{n_1^2} - \frac{1}{n_2^2}\right)$$
where $R$ is the Rydberg constant, $Z$ is the atomic number, $n_1$ is the lower energy level, and $n_2$ is the higher energy level.
Step 1: Set up the ratio for the two ions.
Since the transition is the same for both ions (from $n_2 = 2$ to $n_1 = 1$), the term $R\left(\frac{1}{n_1^2} - \frac{1}{n_2^2}\right)$ is constant for both.
Therefore, the reciprocal of the wavelength is directly proportional to the square of the atomic number ($Z^2$):
$$\frac{1}{\lambda} \propto Z^2 \implies \lambda \propto \frac{1}{Z^2}$$
Step 2: Calculate the ratio of the wavelengths.
For Helium ($He^+$), $Z_{He} = 2$.
For Lithium ($Li^{++}$), $Z_{Li} = 3$.
The ratio of their wavelengths is:
$$\frac{\lambda_{He{\lambda_{Li = \frac{Z_{Li}^2}{Z_{He}^2}$$
Substitute the atomic numbers:
$$\frac{\lambda_{He{\lambda_{Li = \frac{3^2}{2^2} = \frac{9}{4}$$
Thus, the ratio is 9:4.