1966
DOI: 10.1016/0022-3697(66)90004-7
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Kinetics of the alignment of O2− centers in stressed alkali halide crystals

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Cited by 99 publications
(12 citation statements)
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“…Consequently, in the case of a strong linear Jahn-Teller effect at low temperatures the ZPL is described by Eqs. (15) and (16). Therefore, we can conclude that the width and the position of the ZPL in the case of the optical transition A 1 -E with a strong linear Jahn-Teller effect in the E-state depend on temperature according to T 3 and to T 2 ; respectively.…”
Section: Application To a 1 -E Transitionmentioning
confidence: 92%
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“…Consequently, in the case of a strong linear Jahn-Teller effect at low temperatures the ZPL is described by Eqs. (15) and (16). Therefore, we can conclude that the width and the position of the ZPL in the case of the optical transition A 1 -E with a strong linear Jahn-Teller effect in the E-state depend on temperature according to T 3 and to T 2 ; respectively.…”
Section: Application To a 1 -E Transitionmentioning
confidence: 92%
“…The adiabatic potential of the E-state is given by the matrix V 2 in the diagonal representation; it has the form of the Mexican hat [15,[9][10][11]. The vibronic E-state is invariant with respect to the rotation of the q 1 ; q 2 -surface through an arbitrary angle f with the simultaneous rotation of the electronic basis states on the angle 2j: In polar coordinates r ¼ ðq 2 1 þ q 2 2 Þ 1=2 and f ¼ arctanðq 2 =q 1 Þ the adiabatic potentials do not depend on j:…”
Section: A 1 -And E-electronic Statesmentioning
confidence: 99%
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“…Besides the "direct" process, there is a "Raman" process 14,19 in which a phonon is scattered by the impurity, taking up or losing a small amount of energy. Using a Debye model, Pirc, Zeks, and Gosar find for the sum of the direct and Raman processes 19 where T-i=BTil+(T/T 0 n, kT 0 =(2h*ps 5 y /2 /a.…”
Section: ' Lsmentioning
confidence: 99%
“…pro duci ng dyna mi cal inequi valence b etween p otenti al m ini ma. As a result the reori enta ti o n ra te due to the two -phono n Ram an pro cessesb ecomes tem p erature dep endent and pro po rti ona l to À 2 T 3 I 2 ( È D = T ) ; here À i s a tunnel l i ng spli tti ng [11].…”
Section: T R An Sp O R T I N Teg R Als I N M Ol Ecu L Ar D Yn Am I Csmentioning
confidence: 99%