Reorientation Motions of theHA(Li+)Center in KCl:Li+

Abstract
Through a combined electron paramagnetic resonance (EPR) and optical-absorption investigation, it is shown that the HA(Li+) interstitial center in KCl: Li+ exhibits two well-defined motions, the pyramidal motion (P. M.) and the restricted interstitial motion (R. I. M.). The P. M. possesses C4v symmetry around : The Cl2 jumps around a given direction among the four {110} half-planes. This thermally activated motion is responsible for the disorientation temperature TD(P.M.)=23.5 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 TLB(P.M.)=75 K. The P. M. is basically the same as the reorientation motions of the H and HAA centers. The R. I. M. possesses C3v symmetry around : The interstitial Cl exchanges molecular bonds with the three substitutional Cl ions that surround it. This motion is very similar to the VK-center reorientation process. The thermally activated R. I. M. is responsible for the broadening of the EPR lines above TLB(R.I.M.)=29 K, and at 75 K a motionally averaged Cl43 EPR pattern of C3v symmetry is indeed observed. However, in the optical-anisotropy measurements no TD(R.I.M.) 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 HA(Li+6) and HA(Li+7). A few comments are also made on the HA(Na+) center in KCl: Na+.