2019
DOI: 10.1103/physrevb.99.184102
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Spin polarization through intersystem crossing in the silicon vacancy of silicon carbide

Abstract: Silicon carbide (SiC)-based defects are promising for quantum communications, quantum information processing, and for the next generation of quantum sensors, as they feature long coherence times, frequencies near the telecom, and optical and microwave transitions. For such applications, the efficient initialization of the spin state is necessary. We develop a theoretical description of the spin polarization process by using the intersystem crossing of the silicon vacancy defect, which is enabled by a combinati… Show more

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Cited by 28 publications
(19 citation statements)
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“…However, spin-flip processes can still be mediated by non-radiative intersystem crossing involving metastable states, which allows e.g. for deterministic spin state initialisation 21,24 . Note that we do not consider the system's second excited state, V1', whose fluorescence at 858 nm is strongly reduced at cryogenic temperatures due to ultrafast relaxation to the V1 state 20 .…”
Section: Resultsmentioning
confidence: 99%
“…However, spin-flip processes can still be mediated by non-radiative intersystem crossing involving metastable states, which allows e.g. for deterministic spin state initialisation 21,24 . Note that we do not consider the system's second excited state, V1', whose fluorescence at 858 nm is strongly reduced at cryogenic temperatures due to ultrafast relaxation to the V1 state 20 .…”
Section: Resultsmentioning
confidence: 99%
“…This is an indication that both spin states couple to phonons in the same way. A possible explanation is weak spin-orbit coupling [55], but a theoretical consideration of the spin polarization through intersystem crossing [56] involving local vibronic states is necessary to confirm this. Next, we analyze how the change in the V2 PL emission induced by the MW depends on the detection wavelength.…”
Section: Methodsmentioning
confidence: 99%
“…1). A possible reason is that for non-resonant excitation the V3 centers reside in the 4 A 2 state for some time during the excitation-relaxation cycle [42]. Note that the ESLACs in the 4 E octuplet are expected at much higher magnetic fields than those used in our experiments.…”
Section: Temperature Dependence Of Spin Properties a Excited-state Le...mentioning
confidence: 87%