2009
DOI: 10.1002/pssc.200982539
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Luminescence of ZnO crystals under surface and bulk excitation regimes

Abstract: Luminescence properties of vapor phase grown ZnO single crystals with different content of deep traps were explored under one‐photon and two‐photon excitation. Room‐temperature near bandgap emission of highly excited ZnO crystals was originated by inelastic exciton scattering. Under surface excitation regime, luminescence decay profile was governed by exciton diffusion and bimolecular recombination. At higher excitation, exciton recombination transients were significantly altered by stimulated emission. Two‐ph… Show more

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Cited by 4 publications
(3 citation statements)
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“…Band-edge fluorescence of ZnO NRs after 266 nm excitation peaked at about 380 nm (see figure 2(b)), similar to other reported values for ACG-grown ZnO nanorods [27,35], epilayers [36] or bulk crystals [37]. Since the excitation power density was moderately high, the origin of the near-band-edge emission is believed to be inelastic exciton-exciton scattering [37]. One photon excitation creates the high density of excitons in a shallow region of the ZnO NR surface, roughly about…”
Section: Optical Properties Of Zno-nr-coated Surfacessupporting
confidence: 89%
“…Band-edge fluorescence of ZnO NRs after 266 nm excitation peaked at about 380 nm (see figure 2(b)), similar to other reported values for ACG-grown ZnO nanorods [27,35], epilayers [36] or bulk crystals [37]. Since the excitation power density was moderately high, the origin of the near-band-edge emission is believed to be inelastic exciton-exciton scattering [37]. One photon excitation creates the high density of excitons in a shallow region of the ZnO NR surface, roughly about…”
Section: Optical Properties Of Zno-nr-coated Surfacessupporting
confidence: 89%
“…35 From time-resolved PL measurements, b = 10 −10 cm 3 s −1 has been determined for ZnO excitonic recombination. 36 Under the excitation conditions described in Sec. III A., the cores of the highly crystalline particles dictate the CL emission, thus the coefficient value for bulk ZnO was used instead of those for ZnO nanostructures.…”
Section: B Dependence Of Gl Intensities On CL Excitation Powermentioning
confidence: 99%
“…Taking into consideration that the radiative lifetime of excitons in ZnO is about 1 ns at 80 K, 36,38 while the characteristic recombination time of GL varies in the range from 0.2 to 10 ns, 11,31,37 we used τ a = 1 ns and τ b = τ c = 5 ns to keep the problem tractable. In CL measurements, it is more useful to work with the e-h pair generation rate in the electron interaction volume, which, to a first approximation, equals the product of the (average) generation rate G and electron interaction volume.…”
Section: B Dependence Of Gl Intensities On CL Excitation Powermentioning
confidence: 99%