Step 1: Tabulate the low-lying hydrogen levels. Using \(E_n=-13.6/n^2\) eV:
\(E_1=-13.60\) eV, \(E_2=-3.40\) eV, \(E_3=-1.51\) eV, \(E_4=-0.85\) eV, \(E_5=-0.544\) eV.
Step 2: Search for a \(2.55\) eV gap. Absorption of \(2.55\) eV means the difference between the final and initial level equals \(2.55\) eV. Scan the pairs:
\(E_2\to E_3:\ 1.89\) eV; \(E_2\to E_4:\ 2.55\) eV; \(E_1\to E_2:\ 10.2\) eV; \(E_3\to E_4:\ 0.66\) eV.
Only the \(2\to4\) transition matches exactly.
Step 3: Confirm. \(E_4-E_2=(-0.85)-(-3.40)=2.55\) eV, so the sample was initially in state A with \(n=2\) and the absorbed photon lifts electrons to state B with \(n=4\).
Step 4: Consistency note. Since the sample is described as 'a particular excited state', A cannot be the ground state (\(n=1\)); \(n=2\) is indeed an excited state, and \(n=4\) is a further excited state, matching the wording.
\[\boxed{\text{State A}:n=2,\qquad \text{State B}:n=4}\]