Serveur d'exploration sur les relations entre la France et l'Australie

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CHAPTER 12 - Hot Carrier Solar Cells

Identifieur interne : 003C78 ( Main/Exploration ); précédent : 003C77; suivant : 003C79

CHAPTER 12 - Hot Carrier Solar Cells

Auteurs : Gavin Conibeer [Australie] ; Jean-François Guillemoles [Australie] ; Feng Yu [Australie] ; Hugo Levard [Australie]

Source :

RBID : ISTEX:1CA1CBA995053F8D56D16E269A377339F73C3EBD

Descripteurs français

English descriptors

Abstract

The hot carrier cell aims to extract the electrical energy from photogenerated carriers before they thermalize to the band edges. Hence it can potentially achieve a high current and a high voltage and hence very high efficiencies up to 65% under 1 sun. To slow the rate of carrier thermalization is very challenging, but modification of the phonon energies and the use of nanostructures are both promising ways to achieve some of the required slowing of carrier cooling. A number of materials and structures are being investigated with these properties and test structures are being fabricated. It is expected that very soon proof of concept of hot carrier devices will pave the way for their development to fully functioning high efficiency solar cells.

Url:
DOI: 10.1039/9781849739955-00379


Affiliations:


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Le document en format XML

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<term>Appl</term>
<term>Auger</term>
<term>Auger processes</term>
<term>Auger recombination</term>
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<term>Bandgap</term>
<term>Bandgaps</term>
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<term>Carrier population</term>
<term>Carrier temperature</term>
<term>Carrier temperatures</term>
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<term>Double barrier</term>
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<term>Energy dissipation</term>
<term>Energy levels</term>
<term>Energy mater</term>
<term>Escs</term>
<term>European photovoltaic</term>
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<term>Extraction energy</term>
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<term>Figure chapter</term>
<term>Final states</term>
<term>First application</term>
<term>First klemens surface</term>
<term>Flat dispersion relation</term>
<term>Frohlich interaction</term>
<term>Gaas</term>
<term>Guillemoles</term>
<term>Hcsc</term>
<term>Impact ionization</term>
<term>Ionization</term>
<term>Klemens</term>
<term>Klemens channels</term>
<term>Klemens decay</term>
<term>Konig</term>
<term>Large mass</term>
<term>Large phonon bandgap</term>
<term>Lattice</term>
<term>Lattice temperature</term>
<term>Lett</term>
<term>Mass ratio</term>
<term>Matrix</term>
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<term>Modelled</term>
<term>Modelling</term>
<term>Nanostructure</term>
<term>Nanostructures</term>
<term>Narrow range</term>
<term>Nitride</term>
<term>Nozik</term>
<term>Open circuit</term>
<term>Optical phonon</term>
<term>Optical phonon energies</term>
<term>Optical phonons</term>
<term>Optical phonons decay</term>
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<term>Phonon bottleneck</term>
<term>Phonon decay</term>
<term>Phonon dispersion</term>
<term>Phonon energies</term>
<term>Phonon energy</term>
<term>Phonon lifetime</term>
<term>Phonon modes</term>
<term>Phonon modulation</term>
<term>Phononic</term>
<term>Phonons</term>
<term>Photon</term>
<term>Photon energies</term>
<term>Photon energy</term>
<term>Photovoltaics</term>
<term>Phys</term>
<term>Polar semiconductors</term>
<term>Quantum wells</term>
<term>Radiative recombination</term>
<term>Reciprocal space</term>
<term>Recombination</term>
<term>Ridley</term>
<term>Ridley surfaces</term>
<term>Selective emitter</term>
<term>Semiconductor</term>
<term>Shrestha</term>
<term>Solar cell</term>
<term>Thermal equilibrium</term>
<term>Thermalization</term>
<term>Thermalization rate</term>
<term>Thermalization time</term>
<term>Third klemens surface</term>
<term>Triple barrier</term>
<term>Tunnelling</term>
<term>Valence</term>
<term>Valence band</term>
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<front>
<div type="abstract">The hot carrier cell aims to extract the electrical energy from photogenerated carriers before they thermalize to the band edges. Hence it can potentially achieve a high current and a high voltage and hence very high efficiencies up to 65% under 1 sun. To slow the rate of carrier thermalization is very challenging, but modification of the phonon energies and the use of nanostructures are both promising ways to achieve some of the required slowing of carrier cooling. A number of materials and structures are being investigated with these properties and test structures are being fabricated. It is expected that very soon proof of concept of hot carrier devices will pave the way for their development to fully functioning high efficiency solar cells.</div>
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