Download PDF by Michael D. Kaplan: Cooperative Phenomena in Jahn—Teller Crystals

By Michael D. Kaplan

ISBN-10: 1461357551

ISBN-13: 9781461357551

ISBN-10: 1461518598

ISBN-13: 9781461518594

This ebook by means of Kaplan and Vekhter brings jointly the molecular international of the chemist with the condensed topic international of the physicist. sooner than the cave in of the Soviet Union, chemists within the West dedicated lit­ to relationships among molecular digital constitution and tle consciousness solid-state vibronic phenomena. Treating quantum mechanical difficulties in which the adiabatic Born-Oppenheimer approximation fails used to be performed through "brute strength. " With greater and higher desktops to be had within the West, molecular orbital calculations have been performed on saw and conceived static buildings with little trouble for any cooperativity of vibrational habit that may attach those states. whereas it had lengthy been understood within the West that occasions do take place within which varied static constructions are came across for molecules that experience exact or approximately exact digital constructions, little awareness were paid to knowing the vibrational states which may attach such buildings. It used to be more straightforward to calculate the digital constitution saw with a number of attainable distortions than to target how one can couple digital and vibrational habit. within the former Soviet Union, computational energy was once now not as acces­ sible as within the West. a lot larger realization, as a result, used to be dedicated to preserving computational time by means of contemplating basic how you can han­ dle the vibrational connectivity among degenerate or approximately degenerate digital states.

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Extra resources for Cooperative Phenomena in Jahn—Teller Crystals

Example text

This means that terms quadratic in the cubic e mode transform according to Al and E representations, and it is readily perceived that these are the combinations (Q~ + Q~) and (Q~ - Q~, QuQv), respectively. They enter into the vibronic coupling operator as convolutions with the electronic operators 1, T z , and Tx on the basis of the E term and with the operators 1, T u , Tv of the electronic T terms. The situation has one distinctive aspect in that not one but several vibrational modes are transformed according to the representation r, which is active in vibronic mixing.

The situation is more complicated in the majority of real cases, because we have, as a rule, not one but several vibrational modes, which are active in vibronic coupling and are transformed according to the same irreducible representation. For such multimode situations it is very unlikely that any of the limiting cases of weak or strong coupling would occur simultaneously for all active modes; on the other hand, the numerical calculation of multimode problems is virtually impossible. Thus, any real progress in the investigation of such situations is possible only through the use of various simplified models.

Vice versa, if the electron correlation energy increases in vibronic mixing, allowance for these correlations stabilizes the high-symmetry nuclear configuration. 24) that the vibronic contribution grows without bound in the limit x -+ -2. This result looks odd and requires additional investigation. From the physical point of view, as mentioned, the smallness of a ~HF implies a decrease in the energy of the vibron-mixed state as a result of weakening of interelectron repulsion. The equality ~HF = 0 describes the situation when mixing of the ground electronic state with an excited state induces no energy increase whatsoever.

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Cooperative Phenomena in Jahn—Teller Crystals by Michael D. Kaplan

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