Step 1: Recall the Rydberg formula for hydrogen spectrum.
For a transition from higher level \(n_2\) to lower level \(n_1\), the emitted wavelength satisfies:
\[
\frac{1}{\lambda}=R\left(\frac{1}{n_1^2}-\frac{1}{n_2^2}\right)
\]
where \(R\) is the Rydberg constant.
Step 2: Use the wavelength given in the question.
The wavelength is:
\[
\lambda=\frac{36}{5R}
\]
Therefore,
\[
\frac{1}{\lambda}=\frac{5R}{36}
\]
Step 3: Substitute into the Rydberg formula.
So we must have:
\[
R\left(\frac{1}{n_1^2}-\frac{1}{n_2^2}\right)=\frac{5R}{36}
\]
Cancelling \(R\) from both sides:
\[
\frac{1}{n_1^2}-\frac{1}{n_2^2}=\frac{5}{36}
\]
Step 4: Test option \(n=3\) to \(n=2\).
Here \(n_2=3\) and \(n_1=2\). Then:
\[
\frac{1}{n_1^2}-\frac{1}{n_2^2}=\frac{1}{2^2}-\frac{1}{3^2}
\]
\[
=\frac{1}{4}-\frac{1}{9}
\]
\[
=\frac{9-4}{36}=\frac{5}{36}
\]
This exactly matches the required value.
Step 5: Verify that this corresponds to emission.
Since the electron moves from \(n=3\) to \(n=2\), it goes from higher to lower energy level, so light is emitted. Hence the transition is physically correct.
Step 6: Compare with the remaining options.
Since the first option gives the exact factor \(\frac{5}{36}\), there is no need to test further. Therefore, the correct transition is uniquely identified.
Step 7: State the final answer.
Thus, the emitted wavelength \(\frac{36}{5R}\) corresponds to the transition:
\[
\boxed{n=3 \text{ to } n=2}
\]
which matches option \((1)\).