1. Effects of high-energy proton implantation on the luminescence properties of InAs submonolayer quantum dots
- Author
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S. Upadhyay, P. Shete, Subhananda Chakrabarti, Arjun Mandal, Binita Tongbram, Param Jeet Singh, and N.B.V. Subrahmanyam
- Subjects
Photoluminescence ,Materials science ,Proton ,Passivation ,Gaas ,Biophysics ,Analytical chemistry ,02 engineering and technology ,Efficiency ,Growth ,01 natural sciences ,Biochemistry ,Submonolayer Quantum Dots ,0103 physical sciences ,Dark-Current ,010302 applied physics ,Enhancement ,Iii-V Semiconductor ,Ion Implantation ,General Chemistry ,021001 nanoscience & nanotechnology ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,Ion implantation ,Quantum dot ,Infrared Photodetectors ,Molecular Beam Epitaxy ,0210 nano-technology ,Luminescence ,Molecular beam epitaxy ,Dark current - Abstract
Herein, we demonstrate enhancement in photoluminescence (PL) efficiency of InAs submonolayer quantum dots (QDs) resulting from high-energy proton implantation. To obtain optimum energy of protons, we initially varied the energy from 2 MeV to 4.5 MeV at a fixed fluence of 2 x 10(12) ions/cm(2). At an optimum energy of 2.5 MeV, we varied the proton dose from 8 x 10(11) to 1 x 10(13) ions/cm(2) to obtain the best PL response. As compared to the as-grown sample, all implanted samples exhibited PL enhancement, attributed to passivation of non-radiative recombination centers and annihilation of defects, with a consistent blue shift, attributed to out-diffusion of In atoms from the dots. From the PL results, a model was proposed for explaining the material improvement of implanted submonolayer QDs. All samples exhibited significant enhancement in thermal activation energies, confirming that proton implantation improved material quality. Finally, MESA-shaped single-pixel N-i-N detectors were fabricated for both as-grown and optimized samples (implanted with dose of 5 x 10(12) ions/cm(2) at an energy of 2.5 MeV) to measure the temperature-dependent dark current variation. At a temperature of 77 K and a bias of -0.20 V, the dark current density of similar to 4.5 x 10(-4) A/cm(2) of as-grown device was suppressed by more than one order to 6 x 10(-6) A/cm(2) for the optimized sample. (C) 2015 Elsevier B.V. All rights reserved.
- Published
- 2016