2013
DOI: 10.1038/nphys2826
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Room-temperature quantum microwave emitters based on spin defects in silicon carbide

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Cited by 239 publications
(289 citation statements)
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“…4d, showing the overall PL enhancement by a factor of 5.5. This corresponds to N ¼ 3:9Â10 16 cm À 3 and demonstrates that V Si defects can be created at high density in a controlled manner, as required, for instance, for the implementation of a SiC maser 12 .…”
Section: Resultsmentioning
confidence: 77%
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“…4d, showing the overall PL enhancement by a factor of 5.5. This corresponds to N ¼ 3:9Â10 16 cm À 3 and demonstrates that V Si defects can be created at high density in a controlled manner, as required, for instance, for the implementation of a SiC maser 12 .…”
Section: Resultsmentioning
confidence: 77%
“…The dangling bonds of four C atoms with the absent Si atom result in formation of energy levels within the forbidden gap (3.23 eV) of 4H-SiC 24,25 . In case of negatively charged V Si , five electrons form a spin quadruplet (S ¼ 3/2) in the ground state 12,26 . To excite these defects we use sub-band gap excitation of SiC at a laser wavelength of 785 nm (hn ¼ 1.58 eV), which is close to their optimal excitation wavelength 27 .…”
Section: Resultsmentioning
confidence: 99%
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“…These electron spins can be optically initialized and read out [2,6-9], making them very attractive candidates for QIP and related applications [10][11][12]. Among these qubits, silicon-vacancy related defects in hexagonal polytypes of SiC, such as 4H -and 6H -SiC, have shown favorable spin properties [13,14], demonstrated even at a single defect level at room temperature [4]. Two and three different silicon-vacancy related centers were observed in 4H -and 6H -SiC, where the corresponding photoluminescence (PL) lines are denoted as V1 and V2, and V1, V2, and V3, [15,16], respectively.…”
mentioning
confidence: 99%