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Fabrication and optical characterization of ultrathin III-V transferred heterostructures for hot-carrier absorbers

Authors :
Giteau, Maxime
Watanabe, Kentaroh
Miyashita, Naoya
Sodabanlu, Hassanet
Suchet, Daniel
Goffard, Julie
Delamarre, Amaury
Tamaki, Ryo
Jehl, Zacharie
Lombez, Laurent
Sugiyama, Masakazu
Cattoni, Andrea
Collin, Stéphane
Guillemoles, Jean-François
Okada, Yoshitaka
Tokyo University of Science [Tokyo]
Institut Photovoltaïque d’Ile-de-France (UMR) (IPVF)
École polytechnique (X)-Ecole Nationale Supérieure de Chimie de Paris - Chimie ParisTech-PSL (ENSCP)
Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-TOTAL FINA ELF-EDF (EDF)-Institut de Chimie du CNRS (INC)-Centre National de la Recherche Scientifique (CNRS)-Institut Photovoltaïque d’Ile-de-France (ITE) (IPVF)-Air Liquide [Siège Social]
Institut Photovoltaïque d’Ile-de-France (ITE) (IPVF)
Centre de Nanosciences et de Nanotechnologies (C2N)
Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)
Source :
Physics, Simulation, and Photonic Engineering of Photovoltaic Devices IX, Physics, Simulation, and Photonic Engineering of Photovoltaic Devices IX, Feb 2020, San Francisco, France. pp.6, ⟨10.1117/12.2544537⟩
Publication Year :
2020
Publisher :
SPIE, 2020.

Abstract

A hot-carrier solar cell (HCSC) is a high-efficiency photovoltaic concept where electrons and holes are at a higher temperature than the lattice, allowing an additional thermoelectric energy conversion. There are two requirements for a HCSC: establishing a hot-carrier population and converting the temperature into extra voltage through energy-selective contacts. We focus on the generation of hot carriers, and the design of absorbers that can make this generation easier. Fundamentally, this requires to increase the power density absorbed per volume unit, so the photocarriers cannot fully thermalize (phonon bottleneck). Beyond simply increasing the light intensity, the main control knobs to favor hot carriers include reducing the thickness of the absorber, increasing its absorptivity, and reducing its bandgap. In this proceeding, we report the fabrication of structures that aim at measuring the influence of these different parameters. We justify our choices for sample structure and fabrication method from the need for high thermal conductivity, in order to prevent lattice heating. We characterize our structures in order to determine precisely the final thickness of all layers, and the absorptivity of the absorber layer. These samples are to be used for an analysis of the temperature with many variable parameters, in order to better understand the thermalization mechanisms and design better absorbers. Ultimately, our objective is to implement all solutions together in order to evidence a hot carrier population under concentrated sunlight illumination.

Details

Database :
OpenAIRE
Journal :
Physics, Simulation, and Photonic Engineering of Photovoltaic Devices IX
Accession number :
edsair.doi.dedup.....6852fad661fc90f1e63d47517f4663a0