1984
DOI: 10.1002/9780470142813.ch3
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Jahn–Teller Trajectories

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1986
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Cited by 9 publications
(11 citation statements)
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“…However the situation with t 2g electrons in case of strong SOC might be very different from the e⊗E case, just because of a strong spin-orbit entanglement introduced by SOC. And indeed, it is known that for d 1 configuration in case of infinitely strong SOC, where we are dealing with the j = 3/2 quartet, JT coupling to T 2 vibrations still survives [8,10]. The case of intermediate JT coupling, not considered in the previous literature, present special interest because real 4d and 5d systems usually belong to this category.…”
Section: Introductionmentioning
confidence: 98%
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“…However the situation with t 2g electrons in case of strong SOC might be very different from the e⊗E case, just because of a strong spin-orbit entanglement introduced by SOC. And indeed, it is known that for d 1 configuration in case of infinitely strong SOC, where we are dealing with the j = 3/2 quartet, JT coupling to T 2 vibrations still survives [8,10]. The case of intermediate JT coupling, not considered in the previous literature, present special interest because real 4d and 5d systems usually belong to this category.…”
Section: Introductionmentioning
confidence: 98%
“…Such a strong interplay of electronic and lattice characteristics in the systems with spin-orbit entangled states should lead to a plethora of novel quantum phenomena, the analysis of which is now seems to be only at the initial stage. In this connection, let us note some early [2,[8][9][10] and several recent [11][12][13][14][15][16][17][18] papers, but particularly mention unduly rarely cited paper of K.D. Warren [19].…”
Section: Introductionmentioning
confidence: 99%
“…Let r 1 denote the quadratic SO(3) invariant of sl(3, R)/so (3), r 1 (Q) = |Q| 2 = Q, and r 2 (Q) be the cubic. The latter may be obtained from the secular determinant of H JT (Q) [36], or as the totally symmetric SO(3) irrep 0 in the decomposition of the tensor product 2 ⊗ 2 ⊗ 2, since the cubic invariant is a homogeneous polynomial of third degree in the vibrational coordinates [30]. We provide a simple derivation of r 2 (Q) below.…”
Section: A Symmetry-adapted Coordinates and Orbit Spacesmentioning
confidence: 99%
“…Thus, SO(3)-adapted coordinates for the molecular displacements are given by Q = (3) rotations. They can be understood as Euler angles in the space of JT active distorted structures [30,55]. We employ the zyz convention for the parametrization of SO(3) elements,…”
Section: A Symmetry-adapted Coordinates and Orbit Spacesmentioning
confidence: 99%
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