Chemical-potential locking by inter-junction radiative coupling and gap-dependent junction-order inversion in near-field multijunction thermoradiative devices

Thermoradiative (TR) diodes convert low-grade heat into electricity through their own net emission, and two routes have been proposed to raise their output: placing a receiver in the near field and stacking junctions with different band gaps. Multijunction TR analyses so far assume far-field exchange and junctions that do not exchange photons with each other, while near-field multijunction converter models resolve absorption in each subcell but not the emission of subcells at nonzero chemical potential. In a TR stack, however, all junctions share the emitter temperature and differ only in their photon chemical potential, so their mutual near-field exchange can couple their operating points. Modeling this requires layer-resolved emission from every absorbing layer, separation of interband from free-carrier absorption, wave-vector integration up to the inverse spacer thickness, and a two-dimensional voltage optimization. We develop such a model for a HgCdTe/InSb stack at 550 K facing a receiver at 300 K and validate it against published near-field, TR-device, and multijunction results. Inter-junction exchange locks the optimal chemical potentials together, to |μ_f − μ_b| = 10^−3 k_B T_h against 0.93 k_B T_h without it, and lowers the maximum power by factors of 14-55 for a 1-nm spacer. A ratio of inter-junction to junction-receiver radiative conductance predicts the decoupling spacer thickness, 19-69 nm for gaps of 10-100 nm. Wave-vector-resolved transmission maps show how the gap-facing junction screens the buried one, the preferred junction order inverts with gap, and the near field raises the external radiative efficiency of the gap-facing junction 18-fold. In the radiative limit a single junction of equal active thickness always delivers more power; with Auger and Shockley-Read-Hall processes, a thin decoupled stack with the narrow-gap junction in front delivers 51% more power and 74% higher efficiency at a 10-nm gap. In the radiative limit locked junctions lose less than 2% in series or parallel connection, whereas with Auger and SRH processes decoupled junctions lose up to 68% in parallel connection. These results establish inter-junction coupling as a controlling mechanism in near-field multijunction TR devices and give quantitative rules for spacer thickness, junction order, thickness, and electrical connection.

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-11-02
DOI
https://doi.org/10.5281/zenodo.23873420
Primary Topic
Thermal Radiation and Cooling Technologies
Type
preprint
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preprint

Chemical-potential locking by inter-junction radiative coupling and gap-dependent junction-order inversion in near-field multijunction thermoradiative devices

Ehsanur Rahman, Yee Sin Ang
7 links
Zenodo (CERN European Organization for Nuclear Research)
Thermal Radiation and Cooling Technologies
preprint

Chemical-potential locking by inter-junction radiative coupling and gap-dependent junction-order inversion in near-field multijunction thermoradiative devices

Ehsanur Rahman, Yee Sin Ang
preprint en

Abstract

Thermoradiative (TR) diodes convert low-grade heat into electricity through their own net emission, and two routes have been proposed to raise their output: placing a receiver in the near field and stacking junctions with different band gaps. Multijunction TR analyses so far assume far-field exchange and junctions that do not exchange photons with each other, while near-field multijunction converter models resolve absorption in each subcell but not the emission of subcells at nonzero chemical potential. In a TR stack, however, all junctions share the emitter temperature and differ only in their photon chemical potential, so their mutual near-field exchange can couple their operating points. Modeling this requires layer-resolved emission from every absorbing layer, separation of interband from free-carrier absorption, wave-vector integration up to the inverse spacer thickness, and a two-dimensional voltage optimization. We develop such a model for a HgCdTe/InSb stack at 550 K facing a receiver at 300 K and validate it against published near-field, TR-device, and multijunction results. Inter-junction exchange locks the optimal chemical potentials together, to |μ_f − μ_b| = 10^−3 k_B T_h against 0.93 k_B T_h without it, and lowers the maximum power by factors of 14-55 for a 1-nm spacer. A ratio of inter-junction to junction-receiver radiative conductance predicts the decoupling spacer thickness, 19-69 nm for gaps of 10-100 nm. Wave-vector-resolved transmission maps show how the gap-facing junction screens the buried one, the preferred junction order inverts with gap, and the near field raises the external radiative efficiency of the gap-facing junction 18-fold. In the radiative limit a single junction of equal active thickness always delivers more power; with Auger and Shockley-Read-Hall processes, a thin decoupled stack with the narrow-gap junction in front delivers 51% more power and 74% higher efficiency at a 10-nm gap. In the radiative limit locked junctions lose less than 2% in series or parallel connection, whereas with Auger and SRH processes decoupled junctions lose up to 68% in parallel connection. These results establish inter-junction coupling as a controlling mechanism in near-field multijunction TR devices and give quantitative rules for spacer thickness, junction order, thickness, and electrical connection.

Zenodo (CERN European Organization for Nuclear Research)
Jiangnan University (CN), Bangladesh University of Engineering and Technology (BD)
Affordable and clean energy
Thermal Radiation and Cooling Technologies
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