2011
DOI: 10.1103/physrevb.84.115204
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Optical properties of triplet states of excitons bound to interstitial-carbon interstitial-oxygen defects in silicon

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Cited by 3 publications
(8 citation statements)
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“…The strong mixing with λ z spin-orbit coupling in the excited state enables a triplet signal with considerable intensity. According to our spin-orbit calculations, the intensity ratio of the triplet phosphorescence is 1% for the m S = 0 state in the triplet manifold, in good agreement with the experimental findings 31 . This results in about 1.4 ms radiative lifetime for this state.…”
Section: Optical Propertiessupporting
confidence: 90%
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“…The strong mixing with λ z spin-orbit coupling in the excited state enables a triplet signal with considerable intensity. According to our spin-orbit calculations, the intensity ratio of the triplet phosphorescence is 1% for the m S = 0 state in the triplet manifold, in good agreement with the experimental findings 31 . This results in about 1.4 ms radiative lifetime for this state.…”
Section: Optical Propertiessupporting
confidence: 90%
“…It provides a large stabilisation for the m S = 0 level, but is negligible for the other two sublevels, owing to the differences in the energy gaps. Thus, the axial ZFS parameter is modified to D = 5.7 GHz, which is in reasonable agreement with the ~3 GHz readout from the broad peaks in the magneto-PL spectrum 31 . The re-normalisation also leads to a strong mixing of the excited state singlet and triplet m S = 0 levels, manifesting as a 1% contribution of the triplet state to the excited singlet state.…”
Section: Spin Propertiessupporting
confidence: 74%
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“…Therefore, the recombination process is presumably inherently forbidden, for emample, requiring a spin flip from an initial S = 1 state to a S = 0 final state. From “pseudo‐donor”‐type defects in silicon like the C line (a carbon‐oxygen defect emitting at 0.79 eV) it is known, that the deeply bound hole can loosely bind an electron in EMT‐like shallow states and by coupling can form as initial states before recombination either a S = 1 triplet ground state (forbidden) or a S = 0 excited (allowed) state split by ≈2.5 meV . In the present case of the 2.08 eV band, the ultra‐long PL lifetime remains up to room temperature, what would require a singlet‐triplet splitting energy of some 25 meV and therefore appears as unrealistic.…”
Section: Resultsmentioning
confidence: 83%