LOW-TEMPERATURE ABSORPTION AND RESONANCE RAMAN-SPECTRA OF THE MNO4(-)ION DOPED IN A KCLO4 CRYSTAL

Authors
Citation
M. Leuchs et W. Kiefer, LOW-TEMPERATURE ABSORPTION AND RESONANCE RAMAN-SPECTRA OF THE MNO4(-)ION DOPED IN A KCLO4 CRYSTAL, Physical review. B, Condensed matter, 48(21), 1993, pp. 15690-15697
Citations number
27
Categorie Soggetti
Physics, Condensed Matter
ISSN journal
01631829
Volume
48
Issue
21
Year of publication
1993
Pages
15690 - 15697
Database
ISI
SICI code
0163-1829(1993)48:21<15690:LAARRO>2.0.ZU;2-T
Abstract
We have performed polarized absorption and resonance Raman experiments on a permanganate ion doped in a potassium perchlorate single crystal at temperature T = 15 K. At this low temperature the m(C(s)) site spl itting of the excited degenerate 1T2 electronic level of the permangan ate ion is well resolved and the amount of splitting is about 40 cm-1. Due to the clectronic configuration, one would expect that non-Condon terms have to be considered in the description of the absorption spec trum. For the theoretical simulation of our experimental results we ha ve used expressions derived from the time-correlator formulation for t he optical absorption. These are much easier to handle and they cause significant shorter calculation times than the usual sum-over-states e xpressions. In order to determine the symmetries and the wave-number p ositions of the site-split permanganate vibrations, we have performed resonance Raman experiments. The results obtained from these experimen ts form the basis for the interpretation of the absorption spectrum. T he applied model includes the linear and quadratic electron-phonon and linear non-Condon coupling. Within this model we describe the multimo de system and we show how a normal vibration, which apparently has no significant effects in the absorption spectrum, influences the discuss ion of the model system. For the fully symmetric breathing mode of the permanganate ion, we have calculated the change of the Mn-O equilibri um bond length in the electronic excited state from the corresponding linear electron-phonon coupling constant to be 4.6+/-0.4 pm.