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Hot electron light-emitting semiconductor heterostructure device--type 2
Institution:1. Department of Physics, National Institute of Technology Manipur, Langol 795004, India;2. Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India;3. Department of Physics, Assam Don Bosco University, Sonapur 782402, Assam, India;4. CIMPLE-PSI Laboratory, Centre of Plasma Physics-Institute for Plasma Research, Sonapur 782402, Assam, India;5. Institute of Physics, University of Brasília, 70919-970 Brasília, DF, Brazil;6. Department of Materials and Henry Royce Institute, School of Natural Sciences, The University of Manchester, Oxford Road, Manchester M13 9PL, United Kingdom
Abstract:A novel hot electron light-emitting device is proposed which operates by the application of longitudinal electric field, i.e. in the plane of the GaAs quantum wells, which are placed next to the junction plane of an n-Ga1-xAlxAs--p-GaAs heterostructure. Application of high electric fields results in the transfer of hot electrons via tunnelling and thermionic emission, from the quantum well in the depletion region, into the GaAs inversion layer. The hot holes in the p-GaAs, initially away from the junction, then diffuse towards the junction plane to recombine with the excess hot electrons, giving rise to electroluminescence (EL) which is representative of the GaAs band-to-band emission. As the applied field is increased, a high-energy tail in the EL spectrum develops, and, photons with energies greater than the el-hhl transition energy in the quantum well are absorbed and re-emitted by the quantum well. Thus a second peak develops in the EL spectra which becomes stronger with increasing applied electric field. The device has been theoretically modelled, by solving Schrodinger and Poisson's equations self-consistently, to understand the processes leading to EL emission in the various channels.
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