The resolved lines arise from simultaneous changes of vibration and rotation in hydrogen cyanide. A vibrational fundamental connects many populated lower rotational levels to different upper rotational levels, giving the fine structure of a rovibrational spectrum.
The prominent central Q branch, together with flanking P branch and R branch lines, identifies a perpendicular band. For linear HCN, this is the doubly degenerate bending fundamental, not either stretching fundamental. Bending creates a transition-dipole component perpendicular to the molecular axis; its vibrational angular momentum permits as well as .
The two perpendicular bending coordinates share one vibrational frequency. Their degeneracy is different from the series of resolved rotational transitions superimposed on that fundamental. The stretches have their electric dipole transition moment along the molecular axis and would give the usual parallel-band P/R pattern without this strong central Q feature.
This is a rovibrational spectrum: the vibrational excitation is accompanied by quantized molecular rotation. The high-wavenumber R branch has , and the low-wavenumber P branch has . In the simplest common- approximation,
Consecutive lines within either branch are therefore separated by roughly , while the gap between P(1) and R(0) is roughly . There is no Q branch: for this diatomic parallel transition, the electric-dipole rotational selection rule allows , and the line strength vanishes.
The intensity envelope comes from rotational populations, approximately , together with the rotational line strengths. The paired peaks arise from the two chlorine isotopologues, and : their different reduced masses shift both rotational and vibrational spacings. The more abundant gives the stronger member. The changing spacing away from the band centre reflects and, at higher , centrifugal distortion; it is not evidence for additional vibrational fundamentals.