Ap. Smith et al., QUASI-2-DIMENSIONAL QUANTUM STATES OF H-2 IN STAGE-2 RB-INTERCALATED GRAPHITE, Physical review. B, Condensed matter, 53(15), 1996, pp. 10187-10199
Inelastic-incoherent-neutron scattering can be a valuable nanostructur
al probe of H-2-doped porous materials, provided the spectral peaks ca
n be interpreted in terms of crystal-field-split hydrogen-molecule ene
rgy levels, which represent a signature of the local symmetry. Inelast
ic-neutron-scattering measurements as well as extensive theoretical an
alyses have been performed on stage-2 Rb-intercalated graphite (Rb-GIC
), with phys isorbed H-2, HD, and D-2 [composition C(24)M(H-2)(x), wit
h x = 0.8 or 1.0], a layered porous system with abundant spectral peak
s, to assess whether the crystal-field-state picture enables a quantit
ative understanding of the observed structure. The experiments were ma
de at 15 K on the QENS spectrometer at the intense pulsed neutron sour
ce. Potential-energy surfaces for molecular rotational and translation
al motion (parallel and perpendicular to the intercalant plane), as we
ll as the intermolecular interactions of hydrogen molecules in Rb-GIC,
were calculated within local-density-functional theory (LDFT). A root
7 x root 7 periodic unit cell (with composition C28Rb) was treated in
the calculations. Model potentials, parametrized using results of the
LDFT calculations, were employed in schematic calculations of rotatio
nal and translational excited state spectra of a single physisorbed H-
2 molecule in Rb-GIC. Results of our analysis are basically consistent
with the assignment by Stead et al. of the lowest-lying peak at 1.4 m
eV to a rotational-tunneling transition of an isotropic hindered-rotor
oriented normal to the planes, but indicate a small azimuthal anisotr
opy and a lower barrier than for the isotropic case. A peak of low int
ensity at 4.0 meV is most likely a host feature, Based on the experime
ntal isotope shifts and the theoretically predicted states, we conclud
e that spectral peaks at 11 and 22 meV are most likely related to cent
er of mass excitations. We attribute the relatively weak peak at 32 me
V to a librational excitation, and that at 44 meV to an out-of-plane v
ibration.