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Improvement of QDIP performance due to quantum dots with built-in charge
Institution:1. University at Buffalo, The State University of New York, Buffalo, NY 14260, USA;2. Optoelectronic Nanodevices LLC, Amherst, NY 14226, USA;3. Walter Schottky Institut and Physics Department, Technische Universitat München, D-85748 Garching, Germany;1. Institute of Electron Technology, Al. Lotnikow 32/46, 02-668 Warsaw, Poland;2. Institute of Physics Polish Academy of Science, Al. Lotnikow 32/46, 02-668 Warsaw, Poland;1. Dipartimento di Ingegneria Civile, Chimica, Ambientale e dei Materiali, Università di Bologna, Via Terracini 28, 40131 Bologna, Italy;2. Istituto per la Sintesi Organica e la Fotoreattività, CNR, Via Selmi 2, 40126 Bologna, Italy;3. Dipartimento di Ingegneria Industriale, Università di Catania, Viale A. Doria 6, 95125 Catania, Italy;4. Dipartimento di Scienze e Tecnologie Agro-Alimentari, Università di Bologna, Piazza Goidanich, 60 47521 Cesena, Italy;1. Department of Photonics Engineering, Yuan Ze University, 135, Yuan Tung Road, Chungli 320, Taiwan, Republic of China;2. Department of Physics, Fu Jen University, 510, Zhongzheng Road, Xinzhuang District, New Taipei 242, Taiwan, Republic of China;3. Department of Electrical Engineering, Yuan Ze University, 135, Yuan Tung Road, Chungli 320, Taiwan, Republic of China;1. Department of Mathematical and Statistical Sciences, 632 CAB, University of Alberta, Edmonton, AB, T6G 2G1, Canada;2. Department of Pure Mathematics, University of Waterloo, 200 University Ave West, Waterloo, ON, N2L 3G1, Canada
Abstract:The charging of quantum dots provides two strong effects which improve Quantum Dot Infrared Photodetector (QDIP) performance. First, electrons placed in the quantum dots enhance IR-induced transitions and increase electron coupling to IR radiation. Second, the built-in-dot charge creates potential barriers around dots and these barriers strongly suppress the photoelectron capture and exponentially increase the photoelectron lifetime. Both effects enhance the IR photoresponse. Long photoelectron lifetime decreases the generation–recombination noise and increases the device sensitivity. To investigate the potential profiles around charged dots, we used the nextnano3 software which allows for simulation of multilayer structures combined with realistic geometries in one, two, and three spatial dimensions. In weak electric fields the photoelectron kinetics and transport in the potential created by charged dots have been studied analytically. In strong fields the results were based on Monte-Carlo modeling. The effects of dot charging have been investigated in QD structures which were fabricated using molecular beam epitaxy. InAs quantum dots were grown on AlGaAs surfaces by deposition of approximately 2.1 monolayers of InAs. In the obtained structures the dot charging is realized via intra-dot and inter-dot doping. The increase in photoresponse due to dot charging is in good agreement with the model which takes into account anisotropy of potential barriers around QDs in QD layers.
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