Abstract

Kirchhoff’s law of thermal radiation, relating emissivity and absorptance is commonly formulated for opaque bodies in thermodynamic equilibrium with the environment. However, in many systems of practical importance, both assumptions are often not satisfied. We revisit the century-old law and examine the limits of its applicability in an example of Er:YAG and Er:YLF dielectric crystals–potential radiation converters for thermophotovoltaic applications. The (80 at.%) Er:YAG crystal is opaque between 1.45 μm and 1.64 μm. In this spectral range, its absorptance α(λ) is spectrally flat and differentiates from unity only by a small amount of reflection. The shape of the emissivity spectrum ɛ(λ) closely matches that of absorptance α(λ), implying that the Kirchhoff’s law can adequately describe thermal radiation of opaque bodies, even if thermodynamic equilibrium is not satisfied. The (20 at.%) Er:YLF crystal had smaller size, lower concentration of Er ions, and it was not opaque. Nevertheless, its spectrum of emissivity had almost the same shape (between 1.45 μm and 1.62 μm) as the absorptance derived from the transmission measurements. Our results are consistent with the conclusion that the Kirchhoff’s law of thermal radiation can be extended (with caution) to not-opaque bodies away from the thermodynamic equilibrium.

Highlights

  • Two samples used in the thermal radiation studies were Er doped Y3Al5O12 (Er:YAG) and Er doped LiYF4 (Er:YLF)[56, 57]

  • We have shown that the spectra of emissivity ε and absorptance α (at normal incidence) should have identical shapes in optically thin slabs at kabsl ≪ l, without requirement of thermodynamic equilibrium with the environment (only thermalization within the ground state multifold and the excited state multifold is needed)

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Summary

Introduction

(Er:YAG) and Er doped LiYF4 (Er:YLF)[56, 57]. According to the manufacturer[56], the concentration of Er3+ ions in the YAG crystal was equal to 80 at.%. This is consistent with the published spectroscopic data[42, 56]. The Er3+ concentration in the Er:YLF crystal, determined by comparing the absorption spectrum with the literature sources[57], was equal to ~20 at.%. The Er:YAG crystal was too thick to accurately measure the absorption coefficients in the maxima of the spectral lines.

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