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Thermal Emission of Silicon at Near-Infrared Frequencies Mediated by Mie Resonances

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Abstract

Planck’s law constitutes one of the cornerstones in physics. It explains the well-known spectrum of an ideal blackbody consisting of a smooth curve, whose peak wavelength and intensity depend on the temperature of the body. This scenario changes drastically, however, when the size of the emitting object is comparable to the wavelength of the emitted radiation. Here we show that a silicon microsphere (2–3 μm in diameter) heated to around 800 °C yields a thermal emission spectrum consisting of pronounced peaks that are associated with Mie resonances. We experimentally demonstrate in the near-infrared the existence of modes with an ultrahigh quality factor, Q, of 400, which is substantially higher than values reported so far, and set a new benchmark in the field of thermal emission. Simulations predict that the thermal response of the microspheres is very fast, about 15 μs. Additionally, the possibility of achieving light emission above the Planck limit at some frequency ranges is envisaged.

How to cite

Initials first

R. Fenollosa, F. Ramiro-Manzano, M. Garín and R. Alcubilla. Thermal emission of silicon at near-infrared frequencies mediated by Mie resonances. ACS Photonics 6(12), 3174–3179 (2019). DOI: 10.1021/acsphotonics.9b01513.

Family name first

Fenollosa, R., Ramiro-Manzano, F., Garín, M., & Alcubilla, R. (2019). Thermal emission of silicon at near-infrared frequencies mediated by Mie resonances. ACS Photonics, 6(12), 3174–3179. https://doi.org/10.1021/acsphotonics.9b01513

Article access and reuse

The Version of Record is available from ACS Publications and is not hosted on this website. ACS permits authors to reuse their own figures and artwork on personal or institutional websites for non-commercial purposes when the published article is properly cited and any modifications are identified. The four figures below are the unmodified complete compositions extracted from the article PDF.

Figures

Figure 1 from Thermal Emission of Silicon at Near-Infrared Frequencies Mediated by Mie Resonances
Figure 1. Experimental setup and FEM simulation of the temperature distribution and time response of the heating process of a silicon microsphere from room temperature to 750 °C. (a) Schematic of the setup utilized for the experiments, showing how a silicon microsphere supported on a SiO₂ substrate in air is heated by a blue laser and the thermal emission spectrum is collected at a plane parallel to the substrate. (b) Heating (black curve) and cooling (red curve) time evolution of the average temperature of the microsphere upon starting and stopping respectively the irradiation with the blue laser. (c) Cross section view at different scales of the temperature distribution at steady state condition.

© 2019 American Chemical Society. Source: R. Fenollosa et al., ACS Photonics 6(12), 3174–3179 (2019), DOI 10.1021/acsphotonics.9b01513. Reused by the authors on a personal website under the ACS author reuse policy.

Figure 2 from Thermal Emission of Silicon at Near-Infrared Frequencies Mediated by Mie Resonances
Figure 2. Thermal emission spectra of silicon microspheres. (a) Measured spectrum in the NIR for a 3595 nm diameter (Φ) silicon microsphere (black curve in right panel). It agrees with that spectrum obtained from fitting the experimental data to eq 1 (red curve) with a fitted temperature of 756 °C (see Table 1). The calculation indicates that the emission occurs in a much wider range of wavelengths toward the MIR (left panel), and it can reach intensities above the Planck limit (blue curve) at some frequency ranges. The spectra have been plotted against the size parameter, defined as (πΦ/λ), and wavelength. (b) The same as (a) but for a 2308 nm diameter silicon microsphere with a fitted temperature of 841 °C.

© 2019 American Chemical Society. Source: R. Fenollosa et al., ACS Photonics 6(12), 3174–3179 (2019), DOI 10.1021/acsphotonics.9b01513. Reused by the authors on a personal website under the ACS author reuse policy.

Figure 3 from Thermal Emission of Silicon at Near-Infrared Frequencies Mediated by Mie Resonances
Figure 3. Optical absorption parameters for silicon at high temperature. The green curve corresponds to the imaginary part of the refractive index at 756 °C, the temperature of the measurement of Figure 2a. It was obtained from the total absorption coefficient (black curve), which has two main contributions: band gap (blue curve) and free carriers (red curve) that are originated by the temperature and by the pumping laser. For comparison, the dashed red curve shows the absorption produced by the free carriers associated only with temperature. The position of the band gap, Eg, at 756 °C is indicated.

© 2019 American Chemical Society. Source: R. Fenollosa et al., ACS Photonics 6(12), 3174–3179 (2019), DOI 10.1021/acsphotonics.9b01513. Reused by the authors on a personal website under the ACS author reuse policy.

Figure 4 from Thermal Emission of Silicon at Near-Infrared Frequencies Mediated by Mie Resonances
Figure 4. Demonstration of a resonance tuning by temperature and its high Q. (a) Measured resonance TE10,5 of the microsphere of Figure 2a at 756 °C (red dots) and at 792 °C (black dots). The continuous curves correspond to Lorentzian fits that yield a Q of 400 ± 40 in both cases. (b) Electric field intensity distribution of the mode at the resonance plane.

© 2019 American Chemical Society. Source: R. Fenollosa et al., ACS Photonics 6(12), 3174–3179 (2019), DOI 10.1021/acsphotonics.9b01513. Reused by the authors on a personal website under the ACS author reuse policy.