2022
DOI: 10.1126/sciadv.abn7880
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Toward exact predictions of spin-phonon relaxation times: An ab initio implementation of open quantum systems theory

Abstract: Spin-phonon coupling is the main driver of spin relaxation and decoherence in solid-state semiconductors at finite temperature. Controlling this interaction is a central problem for many disciplines, ranging from magnetic resonance to quantum technologies. Spin relaxation theories have been developed for almost a century but often use a phenomenological description of phonons and their coupling to spin, resulting in a nonpredictive tool and hindering our detailed understanding of spin dynamics. Here, we combin… Show more

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Cited by 48 publications
(101 citation statements)
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References 60 publications
(134 reference statements)
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“…The modes with high spin-phonon coupling constants (ν 12 , ν 15 , ν 16 , ν 26 , ν 28 , ν 29 ) also involve more shift in the first coordination sphere, probably due to molecular rotations and delocalized intramolecular distortions (see animated GIF files in SI). 38 Except for these six modes, the impact of spin-phonon coupling on magnetic anisotropy is just nominal (Figure 4). Accordingly for rest of the inspected modes, the corresponding g z values have not been diminished extensively, as reflected by small deviation in the magnitude of second derivatives (g ′ z ) of g z (Table S10 in SI).…”
Section: Spin-phonon Relaxation For Complexmentioning
confidence: 98%
See 1 more Smart Citation
“…The modes with high spin-phonon coupling constants (ν 12 , ν 15 , ν 16 , ν 26 , ν 28 , ν 29 ) also involve more shift in the first coordination sphere, probably due to molecular rotations and delocalized intramolecular distortions (see animated GIF files in SI). 38 Except for these six modes, the impact of spin-phonon coupling on magnetic anisotropy is just nominal (Figure 4). Accordingly for rest of the inspected modes, the corresponding g z values have not been diminished extensively, as reflected by small deviation in the magnitude of second derivatives (g ′ z ) of g z (Table S10 in SI).…”
Section: Spin-phonon Relaxation For Complexmentioning
confidence: 98%
“…Moreover, in order to accomplish and design SMMs operating at higher temperatures, the spin relaxation phenomena via vibronic couplings needs to be deciphered explicitly. 37,38 Therefore, we have attempted to determine the bottleneck effects of spin-vibrational coupling, prominently engendering the spin relaxation, for complex 1 having strong axial magnetic anisotropy.…”
Section: Introductionmentioning
confidence: 99%
“…The vibrational DOS is constructed from uncalibrated harmonic frequencies broadened by antilorentzian line shapes of a constant line width parameter FWHM = 10 cm –1 . Further details, including rate expression for the Orbach and Raman regimes, are given in Section S1. , …”
Section: Computational Detailsmentioning
confidence: 99%
“…39,48 Spin dynamics calculations were carried out using the TAU software, implementing a semiclassical approach used in previous work. 4,8,11,49 Transition rates between different states are obtained by integrating the spin-one-phonon and spin-twophonon rate expressions 50 over the phonon DOS, weighted by Bose−Einstein occupation factors. The spin-phonon matrix elements are evaluated in the equilibrium CFP eigenbasis using CFP derivatives in normal mode coordinates.…”
mentioning
confidence: 99%
“…smaller spin orbit coupling, their relaxation times are longer. 63,65,66 The narrower linewidth also implies that the µw rotor events are more efficient when irradiating the narrow line radical. 36 In addition, for a given magnetic field, MAS frequency and e-e couplings, CE and dipolar-J rotor events are favored thanks to the presence of the narrow line radical.…”
Section: Mas-dnp Field Sweep Profiles and Exchange Distributionmentioning
confidence: 99%