Abstract
The shifts, the relative intensities, and the linewidths of the rotational Raman spectrum of solid parahydrogen (p-H2) and orthodeuterium (o-D2) are calculated by combining the memory-function formalism and a second-order perturbation treatment of the electric-quadrupole–quadrupole interaction. Lattice vibrations are neglected in the present theory. The linewidth is shown to represent the phenomenological T2-dephasing relaxation time, an upper bound of which can be set at ≈600 ps for p-H2 and ≈100 ps for o-D2. It is shown that at low pressure, the present theory compares favorably with the spontaneous Raman measurements on this solid.
| Original language | English |
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| Number of pages | 9 |
| Journal | Physical Review B |
| Volume | 33 |
| Issue number | 6 |
| DOIs | |
| Publication status | Published - 1986 |