2014
DOI: 10.1016/j.jlumin.2013.12.055
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Nanosecond cyclotron resonance in ultrapure diamond

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Cited by 9 publications
(15 citation statements)
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“…These values are shorter than that in the CVD diamond, 1100 ns (blue thin broken line). The faster rise time in each HPHT diamond was caused by the shorter carrier lifetime, as explained by an approximate formula for the rise time [11]. Similar decay behaviors were observed at the magnetic field resonated with heavy hole.…”
Section: Resultssupporting
confidence: 59%
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“…These values are shorter than that in the CVD diamond, 1100 ns (blue thin broken line). The faster rise time in each HPHT diamond was caused by the shorter carrier lifetime, as explained by an approximate formula for the rise time [11]. Similar decay behaviors were observed at the magnetic field resonated with heavy hole.…”
Section: Resultssupporting
confidence: 59%
“…The incident pulse energy was less than 26 μJ corresponding to the incident photon density of b 5.9 × 10 15 photons/cm 3 . In such an excitation density achieved at the wavelength resonated with exciton absorption, carriers were generated by two-body collision of excitons as discussed in our previous paper [11]. Carrier density at the temporal peak after the pulse excitation was estimated to be 3 × 10 11 cm −3 from a spectral shift due to plasma effect.…”
Section: Methodsmentioning
confidence: 92%
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“…Second, the CR signal intensity increased as intensity squared of the incident laser light. These facts indicated that free carriers are generated as a result of a two‐body exciton process (). The density of excitons, estimated based on the incident photon density, was on the order of nex=1016cm −3 .…”
Section: Electron–hole System In Diamond Under Photo‐injectionmentioning
confidence: 99%