TY - JOUR
T1 - Efficiency-optimized near-field thermophotovoltaics using InAs and InAsSbP
AU - Forcade, Gavin P.
AU - Valdivia, Christopher E.
AU - Molesky, Sean
AU - Lu, Shengyuan
AU - Rodriguez, Alejandro W.
AU - Krich, Jacob J.
AU - St-Gelais, Raphael
AU - Hinzer, Karin
N1 - Funding Information:
The authors thank University of Ottawa colleagues C. Zhang and M. Giroux for discussions on this topic. This work was supported in part by the Natural Sciences and Engineering Research Council of Canada (No. NSERC CGS-D) and by the New Frontiers in Research Fund (No. NFRFE-2019-00334). They are also grateful to CMC Microsystems for providing access to the Synopsys Sentaurus software (vS-2021.06).
Publisher Copyright:
© 2022 Author(s).
PY - 2022/11/7
Y1 - 2022/11/7
N2 - Waste heat is a free and abundant energy source, with 15% of global total energy use existing as waste heat above 600 K. For 600-900 K temperature range, near-field thermophotovoltaics (NFTPVs) are theorized to be the most effective technology to recycle waste heat into electrical power. However, to date, experimental efficiencies have not exceeded 1.5%. In this work, we optimize the efficiency of three modeled InAs/InAsSbP-based room-temperature NFTPV devices positioned 0.1 μm from a 750 K p-doped Si radiator. We couple a one-dimensional fluctuational electrodynamics model for the near field optics to a two-dimensional drift-diffusion model, which we validated by reproducing measured dark current-voltage curves of two previously published InAs and InAsSbP devices. The optimized devices show four to six times higher above-bandgap energy transfer compared to the blackbody radiative limit, yielding enhanced power density, while simultaneously lowering parasitic sub-bandgap energy transfer by factors of 0.68-0.85. Substituting InAs front- and back-surface field layers with InAsSbP show 1.5- and 1.4-times higher efficiency and power output, respectively, from lowered parasitic diffusion currents. Of our three optimized designs, the best performing device has a double heterostructure with an n-i-p doping order from front to back. For radiator-thermophotovoltaic gaps of 0.01-10 μm and radiators within 600-900 K, this device has a maximum efficiency of 14.2% and a maximum power output of 1.55 W/cm2, both at 900 K. Within 600-900 K, the efficiency is always higher with near- vs far-field illumination; we calculate up to 3.7- and 107-times higher efficiency and power output, respectively, using near-field heat transfer.
AB - Waste heat is a free and abundant energy source, with 15% of global total energy use existing as waste heat above 600 K. For 600-900 K temperature range, near-field thermophotovoltaics (NFTPVs) are theorized to be the most effective technology to recycle waste heat into electrical power. However, to date, experimental efficiencies have not exceeded 1.5%. In this work, we optimize the efficiency of three modeled InAs/InAsSbP-based room-temperature NFTPV devices positioned 0.1 μm from a 750 K p-doped Si radiator. We couple a one-dimensional fluctuational electrodynamics model for the near field optics to a two-dimensional drift-diffusion model, which we validated by reproducing measured dark current-voltage curves of two previously published InAs and InAsSbP devices. The optimized devices show four to six times higher above-bandgap energy transfer compared to the blackbody radiative limit, yielding enhanced power density, while simultaneously lowering parasitic sub-bandgap energy transfer by factors of 0.68-0.85. Substituting InAs front- and back-surface field layers with InAsSbP show 1.5- and 1.4-times higher efficiency and power output, respectively, from lowered parasitic diffusion currents. Of our three optimized designs, the best performing device has a double heterostructure with an n-i-p doping order from front to back. For radiator-thermophotovoltaic gaps of 0.01-10 μm and radiators within 600-900 K, this device has a maximum efficiency of 14.2% and a maximum power output of 1.55 W/cm2, both at 900 K. Within 600-900 K, the efficiency is always higher with near- vs far-field illumination; we calculate up to 3.7- and 107-times higher efficiency and power output, respectively, using near-field heat transfer.
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U2 - 10.1063/5.0116806
DO - 10.1063/5.0116806
M3 - Article
AN - SCOPUS:85144339225
SN - 0003-6951
VL - 121
JO - Applied Physics Letters
JF - Applied Physics Letters
IS - 19
M1 - 193903
ER -