z-logo
Premium
Investigations of the EPR Zero‐Field Splitting and Local Geometry for Mn 2+ Ion in LiTaO 3 Crystal
Author(s) -
Zheng WenChen
Publication year - 1998
Publication title -
physica status solidi (b)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.51
H-Index - 109
eISSN - 1521-3951
pISSN - 0370-1972
DOI - 10.1002/(sici)1521-3951(199802)205:2<627::aid-pssb627>3.0.co;2-i
Subject(s) - zero field splitting , electron paramagnetic resonance , ion , superposition principle , crystal (programming language) , zero (linguistics) , field (mathematics) , crystal field theory , displacement (psychology) , coupling (piping) , geometry , atomic physics , physics , chemistry , molecular physics , condensed matter physics , materials science , nuclear magnetic resonance , quantum mechanics , electron , mathematics , spin polarization , psychology , linguistics , philosophy , computer science , pure mathematics , metallurgy , psychotherapist , programming language
The EPR zero‐field splitting D for the Mn 2+ ion in LiTaO 3 crystal has been studied from the microscopic spin–orbit coupling mechanism and the empirical superposition model. From the studies, one can find that to reach a good fit between theory and experiment, the Mn 2+ ion does not occupy the exact site of the replaced Li + ion, but is required to move about 0.022(1) nm in the direction of the c ‐axis in the LiTaO 3 crystal. The result and the reasonableness of the displacement direction are discussed. It appears that both theoretical methods can be used to explain the zero‐field splitting of 3d 5 ions in crystals, or, in reverse, to study the local geometry of these ions in crystals from the EPR data.

This content is not available in your region!

Continue researching here.

Having issues? You can contact us here