Reaching 28% Efficiency in Thermo-Photovoltaics
Gregg Scranton a b, Zunaid Omair a b, Luis Pazos-Outón a, T. Patrick Xiao a, Vidya Ganapati c, Myles Steiner d, Per Peterson e, John Holzrichter f, Eli Yablonovitch a b
a Electrical Engineering and Computer Sciences, University of California, Berkeley, Berkeley, California 94720, EE. UU., Berkeley, United States
b Material Sciences Division, Lawrence Berkeley National Laboratory, US, Berkeley, California 94720, United States
c Swarthmore College, Swarthmore, Pennsylvania, USA
d National Renewable Energy Laboratory, Golden, Colorado, 1617 Cole Boulevard, Golden, Colorado, 80401, United States
e Department of Nuclear Engineering, University of California at Berkeley
f Physical Insight Associates, Berkeley, California, USA
Materials for Sustainable Development Conference (MATSUS)
Proceedings of nanoGe Fall Meeting 2018 (NFM18)
S9 Advanced PV Technologies and Concepts with New Functionalities
Torremolinos, Spain, 2018 October 22nd - 26th
Organizers: Joaquim Puigdollers and Alejandro Perez-Rodriguez
Invited Speaker, Luis Pazos-Outón, presentation 003
DOI: https://doi.org/10.29363/nanoge.nfm.2018.003
Publication date: 6th July 2018

Photovoltaic (PV) cells are efficient heat engines, converting incident photon energy to electrical energy. In the case of solar PV, the cell receives radiation from the Sun – which can be approximated as a black body at 5500oC – and converts part of the received radiation to electricity. In an ideal solar PV cell, the maximum energy conversion efficiency is ~33.5%, the famous Shockley-Queisser limit. Entropic losses, thermalization, and unused below-bandgap photons are the main limits of solar PV.

If instead of relying on the Sun, a local black body is used as the source of photons, many of the limitations mentioned can be minimized. This idea, known as thermo-photovoltaics (TPV), has been known since 1960. With a local thermal emitter at a suitable temperature these losses can be minimized and high efficiencies are attainable. Previous efforts have attempted to tune the emissivity spectrum of the emitter, minimizing the amount of below‑bandgap radiation reaching the photovoltaic cell.  This approach, however, bring some challenges due to the difficulty of developing a high quality spectral filter that remains stable at high temperatures.

We report on a thermo‑photovoltaic device that relies on the band‑edge of a photovoltaic absorber to spectrally filter the incoming radiation. Photons above the bandgap are converted to electricity, while the unused and unabsorbed photons below the bandgap are reflected by a ~94% reflective rear electrode and recovered by the source of radiation. Our system uses graphite as the blackbody emitter, and In0.55Ga0.45As (bandgap of 0.74eV) as the photovoltaic absorber.  For an emitter temperature of ~1200°C, we report a power conversion efficiency of 28.1%.

© FUNDACIO DE LA COMUNITAT VALENCIANA SCITO
We use our own and third party cookies for analysing and measuring usage of our website to improve our services. If you continue browsing, we consider accepting its use. You can check our Cookies Policy in which you will also find how to configure your web browser for the use of cookies. More info