Room-temperature ultraviolet luminescence from γ-CuCl grown on near lattice-matched silicon

被引:0
|
作者
O'Reilly, L. [1 ]
Lucas, O.F. [1 ]
McNally, P.J. [1 ]
Reader, A. [1 ,3 ]
Natarajan, Gomathi [1 ]
Daniels, S. [1 ]
Cameron, D.C. [1 ,4 ]
Mitra, A. [2 ]
Martinez-Rosas, M. [2 ,5 ]
Bradley, A.L. [2 ]
机构
[1] Nanomaterials Processing Laboratory, School of Electronic Engineering, Dublin City University, Dublin 9, Ireland
[2] Semiconductor Photonics, Physics Department, Trinity College, Dublin 2, Ireland
[3] Innos Ltd., Faculty of Electronics and Computing, University of Southampton, Highfield, Southampton SO17 1BJ, United Kingdom
[4] Advanced Surface Technology Research Laboratory (ASTRaL), Lappeenranta University of Technology, P.O. Box 181, 50101 Mikkeli, Finland
[5] Universidad Autónoma de Baja California, Ensenada, Mexico
来源
Journal of Applied Physics | 2005年 / 98卷 / 11期
关键词
Crystal lattices - Gamma rays - Luminescence - Optoelectronic devices - Silicon - Ultraviolet radiation;
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摘要
We have probed the luminescence properties of a wide-band-gap, direct band-gap optoelectronic material, grown on closely lattice-matched silicon substrates, namely, γ-CuCl on Si. This material system is compatible with current Si or GaAs-based electronic/optoelectronic technologies. Polycrystalline epitaxy of CuCl can be controlled such that it maintains an orientation similar to the underlying Si substrate. Importantly, chemical interactions between CuCl and Si are eliminated. Photoluminescence and cathodoluminescence results for CuCl, deposited on either Si (100) or Si (111), reveal a strong room-temperature Z3 excitonic emission at ∼387 nm. We have developed and demonstrated the room-temperature operation of an ultraviolet electroluminescent device fabricated by the growth of γ-CuCl on Si. The application of an electrical potential difference across the device results in an electric field, which promotes light emission through hot-electron impact excitation of electron-hole pairs in the γ-CuCl. Since the excitonic binding energy in this direct band-gap material is of the order of 190 meV at room temperature, the electron-hole recombination and subsequent light emission at ∼380 and ∼387 nm are mediated by excitonic effects. © 2005 American Institute of Physics.
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