Reorientation Motions of theCenter in KCl:
- 15 June 1972
- journal article
- research article
- Published by American Physical Society (APS) in Physical Review B
- Vol. 5 (12) , 4970-4986
- https://doi.org/10.1103/physrevb.5.4970
Abstract
Through a combined electron paramagnetic resonance (EPR) and optical-absorption investigation, it is shown that the interstitial center in KCl: exhibits two well-defined motions, the pyramidal motion (P. M.) and the restricted interstitial motion (R. I. M.). The P. M. possesses symmetry around : The jumps around a given direction among the four {110} half-planes. This thermally activated motion is responsible for the disorientation temperature K, around which all optical anisotropy produced at 4.2 K with polarized light disappears, and for the lifetime broadening of the EPR lines above K. The P. M. is basically the same as the reorientation motions of the and centers. The R. I. M. possesses symmetry around : The interstitial Cl exchanges molecular bonds with the three substitutional ions that surround it. This motion is very similar to the -center reorientation process. The thermally activated R. I. M. is responsible for the broadening of the EPR lines above K, and at 75 K a motionally averaged EPR pattern of symmetry is indeed observed. However, in the optical-anisotropy measurements no is observed. It is concluded that the R. I. M. does not freeze in at low temperatures but goes over into a tunneling motion. As a result no optical anisotropy can be produced at 4.2 K with polarized light. No differences have been observed so far for the R. I. M. and the P. M. between and . A few comments are also made on the center in KCl: .
Keywords
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