Enhanced Photon Utilization in Single Cavity Mode Air-Bridge Thermophotovoltaic Cells AITranslate
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An air-bridge thermophotovoltaic (TPV) cell can enable nearly complete utilization of out-of-band (OOB) photons. However, the air-bridge consists of a micron-thick free-standing semiconductor membrane that can buckle during fabrication. Such a buckled membrane supports multiple optical cavity modes in the air gap between the semiconductor and the bottom, metal back surface reflector, causing up to 10% loss in OOB reflectance (ROOB). Here we demonstrate a single cavity mode with an extremely flat In0.53Ga0.47As TPV membrane that exhibits ROOB = 98.9 ± 0.1% under 1279 K blackbody illumination. The remaining 1.1% reflectance loss is attributed to free carrier absorption and cavity oscillations. The flat TPV cell exhibits a spectral efficiency ranging from 68.6% to 76.5% for emitter temperatures between 900 and 1500 K, which exceeds that of previous reflective TPV cells, and represents a 20–30% improvement compared to the buckled cell, leading to a power conversion efficiency of 31.7 ± 0.1% at 1279 K.
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DOI:https://doi.org/10.1021/acsenergylett.3c00720
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An air-bridge thermophotovoltaic (TPV) cell can enable nearly complete utilization of out-of-band (OOB) photons. However, the air-bridge consists of a micron-thick free-standing semiconductor membrane that can buckle during fabrication. Such a buckled membrane supports multiple optical cavity modes in the air gap between the semiconductor and the bottom, metal back surface reflector, causing up to 10% loss in OOB reflectance (ROOB). Here we demonstrate a single cavity mode with an extremely flat In0.53Ga0.47As TPV membrane that exhibits ROOB = 98.9 ± 0.1% under 1279 K blackbody illumination. The remaining 1.1% reflectance loss is attributed to free carrier absorption and cavity oscillations. The flat TPV cell exhibits a spectral efficiency ranging from 68.6% to 76.5% for emitter temperatures between 900 and 1500 K, which exceeds that of previous reflective TPV cells, and represents a 20–30% improvement compared to the buckled cell, leading to a power conversion efficiency of 31.7 ± 0.1% at 1279 K.
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| GB/T 7714-2015 | [1] Jihun Lim, Bosun RoyLayinde, Bin Liu, et al. ACS Energy Letters, 2023(8). DOI:10.1021/acsenergylett.3c00720. |
| MLA | [1] Jihun Lim, et al., ACS Energy Letters, no. 8, 2023, https://doi.org/10.1021/acsenergylett.3c00720. |
| APA | [1] Jihun Lim, Bosun RoyLayinde, Bin Liu, Andrej Lenert, & Stephen R. Forrest. (2023). ACS Energy Letters(8). https://doi.org/10.1021/acsenergylett.3c00720 |
| IEEE | [1] Jihun Lim, Bosun RoyLayinde, Bin Liu, Andrej Lenert, and Stephen R. Forrest, ACS Energy Letters, no. 8, 2023, doi: 10.1021/acsenergylett.3c00720. |
