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Autores principales: Yablonovitch, Eli, Omair, Zunaid
Formato: Preprint
Publicado: 2024
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Acceso en línea:https://arxiv.org/abs/2405.08835
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author Yablonovitch, Eli
Omair, Zunaid
author_facet Yablonovitch, Eli
Omair, Zunaid
contents It has gradually been recognized that incoming sunlight can be trapped within a high refractive index semiconductor, n~3.5, owing to the narrow 16degree escape cone. The solar light inside a semiconductor is 4n^2 times brighter than incident sunlight. This is called light trapping and has increased the theoretical and practical efficiency of solar panels. But there is a second photon gas of equal importance that has been overlooked. Inside every forward-biased solar cell there is a gas of infrared luminescence photons, also trapped by total internal reflection. We introduce the idea of super-equilibrium, when the luminescence photon gas freely exchanges energy with the two quasi-Fermi levels. Nonetheless, the loss of a single photon from either gas is equivalent to the loss of a precious minority carrier. Therefore optical modeling & design becomes equally important as electron-hole modeling in high efficiency solar cells. It becomes possible to approach the idealistic Shockley-Queisser limit, by proper material selection and design of the solar cell optics.
format Preprint
id arxiv_https___arxiv_org_abs_2405_08835
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle There Are Two Distinct Photon Gases Present Inside Every Solar Cell
Yablonovitch, Eli
Omair, Zunaid
Optics
Other Condensed Matter
It has gradually been recognized that incoming sunlight can be trapped within a high refractive index semiconductor, n~3.5, owing to the narrow 16degree escape cone. The solar light inside a semiconductor is 4n^2 times brighter than incident sunlight. This is called light trapping and has increased the theoretical and practical efficiency of solar panels. But there is a second photon gas of equal importance that has been overlooked. Inside every forward-biased solar cell there is a gas of infrared luminescence photons, also trapped by total internal reflection. We introduce the idea of super-equilibrium, when the luminescence photon gas freely exchanges energy with the two quasi-Fermi levels. Nonetheless, the loss of a single photon from either gas is equivalent to the loss of a precious minority carrier. Therefore optical modeling & design becomes equally important as electron-hole modeling in high efficiency solar cells. It becomes possible to approach the idealistic Shockley-Queisser limit, by proper material selection and design of the solar cell optics.
title There Are Two Distinct Photon Gases Present Inside Every Solar Cell
topic Optics
Other Condensed Matter
url https://arxiv.org/abs/2405.08835