2017
DOI: 10.1103/physrevb.96.094431
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Magnetic field induced tunneling and relaxation between orthogonal configurations in solids and molecular systems

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Cited by 14 publications
(33 citation statements)
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“…In ref. , the increase of τnormalB1true(Btrue) with B from 0 to 0.1 T was interpreted as due to a new channel of relaxation via tunneling from one distorted configuration of the JTE center to another one, made possible by the magnetic field‐induced coupling between their otherwise orthogonal orbital states. The decrease from 0.1 to 2 T was explained as due to the change of the attenuation mechanism with the relaxation replaced by quasi‐resonance transitions between greatly broadened energy levels, so that only decaying tail‐resonance dependence is seen.…”
Section: Magnetic Field‐dependent Relaxation Timementioning
confidence: 79%
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“…In ref. , the increase of τnormalB1true(Btrue) with B from 0 to 0.1 T was interpreted as due to a new channel of relaxation via tunneling from one distorted configuration of the JTE center to another one, made possible by the magnetic field‐induced coupling between their otherwise orthogonal orbital states. The decrease from 0.1 to 2 T was explained as due to the change of the attenuation mechanism with the relaxation replaced by quasi‐resonance transitions between greatly broadened energy levels, so that only decaying tail‐resonance dependence is seen.…”
Section: Magnetic Field‐dependent Relaxation Timementioning
confidence: 79%
“…We assume that the magnetic field induces a new channel of relaxation (similar to ref. ). It means that the relaxation rate should be written as follows τ(T,B)1τT,B1=τnormalT1+τnormalB1 where τ B is the part of relaxation time induced by the magnetic field only, and τ T is the temperature‐dependent relaxation time defined at B = 0.…”
Section: Magnetic Field‐dependent Relaxation Timementioning
confidence: 99%
“…Cr atoms substitute Zn atoms in the cubic ZnSe crystal resulting in its ground electronic 5 T 2 state, which can be characterized by the effective orbital momentum L = 1 and total spin S = 2. The orbital states |x,|y,|z of the center couple with local doubly degenerated e ‐symmetry displacements of the four near‐neighbor Se atoms of the tetrahedral environment, resulting in the T⊗e JT problem . The adiabatic potential energy surface (APES) of the CrSe 4 center in the space of normal coordinates Q 2 , Q 3 of the nuclear displacements in this case has three equivalent minima in which the system is distorted along one of the three axes x, y, z , respectively; they correspond to distortions along the [100], [010], and [001] directions of the crystal.…”
Section: Theorymentioning
confidence: 99%
“…The matrix in Equation shows that there is a splitting of the orbital states |x and |y, while the ultrasound wave does not affect the state |z. The diagonal character of the Hamiltonian (Equation ) means that the interaction of the ultrasonic wave propagating along [110] is not affected by the vibronic reduction factors, which are proportional to the overlap of the vibrational functions of two minima of the APES, ϕi|ϕj, ij.…”
Section: Theorymentioning
confidence: 99%
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