We have carried out a computational study of the inelastic electron tunneling
spectrum (IETS) of the two vibrational modes of a single hydrogen atom on a
Cu(100) surface in a scanning tunneling microscopy (STM) junction. This study
addresses key issues about vibrational assignment and line shape of observed
peaks in IETS within the framework of density functional theory calculations
and the Lorente-Persson theory for STM-IETS. We argue that the observation of
only a single, broad peak in the STM-IETS [L.J. Lauhon and W. Ho, Phys. Rev.
Lett. 85, 4566 (2000)] is not caused by any symmetry restrictions or any
cancellation between inelastic and elastic vibrational contributions for one of
the two modes but is due to strongly overlapping superposition of the
contributions from the two modes caused by the rather large instrumental
broadening and the narrow vibrational energy separation between the modes. In
particular, we find that this broadening and the large asymmetry of the
vibrational line shapes gives rise to substantial apparent vibrational energy
shifts of the two modes and decrease their apparent energy separation