2006
DOI: 10.1016/j.jlumin.2006.01.003
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Dynamics of high-density excitons and electron–hole plasma in ZnO epitaxial thin films

Abstract: Time-resolved luminescence spectra due to an electron-hole plasma (EHP emission) and an exciton-exciton scattering process (P emission) were measured in ZnO epitaxial thin films under band-to-band excitation by the optical Kerr gate method. We find that both the EHP and P emissions emerge with a long time delay of a few picoseconds. The time delay observed decreases quadratically with the excitation density below the critical Mott density. These results imply that the P (EHP) emission emerges after completing … Show more

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Cited by 26 publications
(11 citation statements)
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“…These sub-picosecond TRPL measurements are consistent with previous reports where stimulated emission dynamics of ZnO nanostructures were related to carrier densities and the interplay of E-E scattering versus EHP (9)(10)(11). Here we observe the decay time of stimulated emission from EHP to be faster than that from E-E, but that it increases and saturates with increasing pump fluence.…”
Section: Data On Uv Laser Cavitiessupporting
confidence: 92%
“…These sub-picosecond TRPL measurements are consistent with previous reports where stimulated emission dynamics of ZnO nanostructures were related to carrier densities and the interplay of E-E scattering versus EHP (9)(10)(11). Here we observe the decay time of stimulated emission from EHP to be faster than that from E-E, but that it increases and saturates with increasing pump fluence.…”
Section: Data On Uv Laser Cavitiessupporting
confidence: 92%
“…On the other hand, high-density excitation effects on nonmagnetic semiconductors have been well studied [3][4][5][6], such as multi-excitons or electron-hole plasma. Recently, there are a few works on the high-density excitation effect of semimagnetic semiconductor CdMnTe [7,8].…”
Section: Introductionmentioning
confidence: 99%
“…INTRODUCTION Zinc oxide (ZnO) is an ideal material for blue-to-near-UV lasing, 1,2 because it possesses a large direct bandgap of 3.37 eV at room temperature and exhibits a large exciton binding energy of 60 meV. [6][7][8] An additional practical advantage is that the growth of ZnO does not require toxic precursors to yield uniform and high-quality ZnO nanostructures. [6][7][8] An additional practical advantage is that the growth of ZnO does not require toxic precursors to yield uniform and high-quality ZnO nanostructures.…”
mentioning
confidence: 99%