Abstract

We analyze the effect of doping on photoelectron kinetics in quantum dot [QD] structures and find two strong effects of the built-in-dot charge. First, the built-in-dot charge enhances the infrared [IR] transitions in QD structures. This effect significantly increases electron coupling to IR radiation and improves harvesting of the IR power in QD solar cells. Second, the built-in charge creates potential barriers around dots, and these barriers strongly suppress capture processes for photocarriers of the same sign as the built-in-dot charge. The second effect exponentially increases the photoelectron lifetime in unipolar devices, such as IR photodetectors. In bipolar devices, such as solar cells, the solar radiation creates the built-in-dot charge that equates the electron and hole capture rates. By providing additional charge to QDs, the appropriate doping can significantly suppress the capture and recombination processes via QDs. These improvements of IR absorption and photocarrier kinetics radically increase the responsivity of IR photodetectors and photovoltaic efficiency of QD solar cells.

Highlights

  • One of the main goals for the generation of infrared [IR] imaging systems and solar cell photovoltaic devices is to increase the photoresponse to IR radiation [1]

  • We have reported a radical improvement on the responsivity of QD infrared photodetectors [QDIP] [10] and QD solar cell efficiency [11] due to strong inter-dot doping, which creates substantial builtin-dot charge

  • We study the potential relief created by the built-in-dot charge and calculate potential barriers, which separate the conducting states in the media from the localized QD states

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Summary

Introduction

One of the main goals for the generation of infrared [IR] imaging systems and solar cell photovoltaic devices is to increase the photoresponse to IR radiation [1]. We conclude that in both cases, the built-in-dot charge strongly enhances electron coupling to electromagnetic radiation and suppresses the most effective capture processes. These two factors allow us to improve the performance of QDIPs and QD solar cells. To calculate the built-in-dot charge and investigate the potential profiles around dots, we used the nextnano software, which allows for simulation of multilayer structures combined with different materials of realistic geometries in one, two, and three spatial dimensions [13] This simulation tool self-consistently solves Schrödinger, Poisson, and current equations for electrons and holes.

B53 Inter-dot
Conclusions
Findings
15. Bonch-Bruevich VL

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