2019
DOI: 10.1039/c9cp03584b
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Hamiltonian formalism of spin–orbit Jahn–Teller and pseudo-Jahn–Teller problems in trigonal and tetragonal symmetries

Abstract: A formalism for expansions of all bimodal spin–orbit Jahn–Teller and pseudo-Jahn–Teller Hamiltonian operators in trigonal and tetragonal symmetries is presented.

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Cited by 12 publications
(17 citation statements)
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“…So far, we have successfully derived arbitrarily high order expansion formulas for all bimodal JT/pJT problems in trigonal symmetries, 43,44 tetragonal symmetries, 45 cubic group symmetries, 46,47 and spin-orbit JT/pJT problems in trigonal and tetragonal symmetries. 48 These formalisms are inclusive, yet not enough. Problems with more than two sets of JT/pJT active vibrational modes and of higher axial symmetries, e.g., pentagonal (cyclopentadienyl ring 49,50 ), hexagonal (benzene 51,52 ), and in general n-gonal (nanotubes, nanohoops, and nanoloops of different sizes [53][54][55][56] ), await to be addressed.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…So far, we have successfully derived arbitrarily high order expansion formulas for all bimodal JT/pJT problems in trigonal symmetries, 43,44 tetragonal symmetries, 45 cubic group symmetries, 46,47 and spin-orbit JT/pJT problems in trigonal and tetragonal symmetries. 48 These formalisms are inclusive, yet not enough. Problems with more than two sets of JT/pJT active vibrational modes and of higher axial symmetries, e.g., pentagonal (cyclopentadienyl ring 49,50 ), hexagonal (benzene 51,52 ), and in general n-gonal (nanotubes, nanohoops, and nanoloops of different sizes [53][54][55][56] ), await to be addressed.…”
Section: Introductionmentioning
confidence: 99%
“…These pioneering studies motivated us to derive JT/pJT expansion formulas that are of arbitrarily high orders and are as inclusive as for one class of symmetries, instead of one symmetry. So far, we have successfully derived arbitrarily high order expansion formulas for all bimodal JT/pJT problems in trigonal symmetries, , tetragonal symmetries, cubic group symmetries, , and spin–orbit JT/pJT problems in trigonal and tetragonal symmetries . These formalisms are inclusive, yet not enough.…”
Section: Introductionmentioning
confidence: 99%
“…So far, we have successfully derived arbitrarily high order expansion formulas for all bimodal JT/pJT problems in trigonal symmetries, 43,44 tetragonal symmetries, 45 cubic group symmetries, 46,47 and spin-orbit JT/pJT problems in trigonal and tetragonal symmetries. 48 These formalisms are inclusive, yet not enough. Problems with more than two sets of JT/pJT active vibrational modes and of higher axial symmetries, e.g., pentagonal (cyclopentadienyl ring 49,50 ), hexagonal (benzene 51,52 ), and in general n-gonal (nanotubes, nanohoops, and nanoloops of different sizes [53][54][55][56] ), await to be addressed.…”
Section: Introductionmentioning
confidence: 99%
“…So far, we have successfully derived arbitrarily high order expansion formulas for all bimodal JT/pJT problems in trigonal symmetries, 43,44 tetragonal symmetries, 45 cubic group symmetries, 46,47 and spin-orbit JT/pJT problems in trigonal and tetragonal symmetries. 48 These formalisms are inclusive, yet not enough. Problems with more than two sets of JT/pJT active vibrational modes and of higher axial symmetries, e.g., pentagonal (cyclopentadienyl ring 49,50 ), hexagonal (benzene 51,52 ), and in general n-gonal (nanotubes, nanohoops, and nanoloops of different sizes [53][54][55][56] ), await to be addressed.…”
Section: Introductionmentioning
confidence: 99%