
1.State Key Laboratory of ASIC and System, Centre of Micro-Nano System, SIST, Fudan University, 200433, Shanghai, China
2.Department of Physics, Government Postgraduate College, (Higher Education Department-HED) Khyber Pakhtunkhwa, 21300, Mansehra, Pakistan
3.State Key Laboratory of Surface Physics, Key Laboratory of Micro- and Nano-Photonics, Fudan University, 200433, Shanghai, China
4.Faculty of Engineering and Natural Sciences, Tampere University, FI-33014, Tampere, Finland
5.KAUST Solar Center, Division of Physical Science and Engineering, King Abdullah University of Science and Technology (KAUST), Thuwal, 23955-6900, Riyadh, Kingdom of Saudi Arabia
rfan Ahmed (swateez.scme.nust@gmail.com)
Yiqiang Zhan (yqzhan@fudan.edu.cn)
Published:30 September 2021,
Published Online:01 September 2021,
Received:08 March 2021,
Revised:22 July 2021,
Accepted:31 July 2021
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Ahmed I. et al. There is plenty of room at the top: generation of hot charge carriers and their applications in perovskite and other semiconductor-based optoelectronic devices. Light: Science & Applications, 10, 1630-1657 (2021).
Ahmed I. et al. There is plenty of room at the top: generation of hot charge carriers and their applications in perovskite and other semiconductor-based optoelectronic devices. Light: Science & Applications, 10, 1630-1657 (2021). DOI: 10.1038/s41377-021-00609-3.
Hot charge carriers (HC) are photoexcited electrons and holes that exist in nonequilibrium high-energy states of photoactive materials. Prolonged cooling time and rapid extraction are the current challenges for the development of future innovative HC-based optoelectronic devices
such as HC solar cells (HCSCs)
hot energy transistors (HETs)
HC photocatalytic reactors
and lasing devices. Based on a thorough analysis of the basic mechanisms of HC generation
thermalization
and cooling dynamics
this review outlines the various possible strategies to delay the HC cooling as well as to speed up their extraction. Various materials with slow cooling behavior
including perovskites and other semiconductors
are thoroughly presented. In addition
the opportunities for the generation of plasmon-induced HC through surface plasmon resonance and their technological applications in hybrid nanostructures are discussed in detail. By judiciously designing the plasmonic nanostructures
the light coupling into the photoactive layer and its optical absorption can be greatly enhanced as well as the successful conversion of incident photons to HC with tunable energies can also be realized. Finally
the future outlook of HC in optoelectronics is highlighted which will provide great insight to the research community.
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