Abstract

The control of thermal emission spectra using optical resonances has been attracting increased attention both with respect to fundamental science and for various applications, including infrared sensing, thermal imaging, and thermophotovoltaics. In this mini-review, we describe the recent experimental demonstrations of narrowband thermal emission with optical nanostructures, including metallic cavities, metamaterials, and all-dielectric photonic crystals. The spectral features of the controlled thermal emission (e.g., wavelength, linewidth, peak emissivity, and angular characteristics) are strongly dependent on the choice of both materials and structures of the emitters. Through the appropriate design of optical nanostructures, arbitrary shaping of thermal emission spectra, from single-peak ultra-narrowband (Q>100) emission for midinfrared sensing to a stepwise emissivity spectrum for thermophotovoltaics, has been successfully realized.

© 2015 Optical Society of America

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2014 (6)

A. Lenert, D. M. Bierman, Y. Nam, W. R. Chan, I. Celanovic, M. Soljačić, E. N. Wang, “A nanophotonic solar thermophotovoltaic device,” Nat. Nanotechnol. 9, 126–130 (2014).
[Crossref]

H. T. Miyazaki, T. Kasaya, M. Iwanaga, B. Choi, Y. Sugimoto, K. Sakoda, “Dual-band infrared metasurface thermal emitter for CO2 sensing,” Appl. Phys. Lett. 105, 121107 (2014).
[Crossref]

W. Streyer, S. Law, A. Rosenberg, C. Roberts, V. A. Podolskiy, A. J. Hoffman, D. Wasserman, “Engineering absorption and blackbody radiation in the far-infrared with surface phonon polaritons on gallium phosphide,” Appl. Phys. Lett. 104, 131105 (2014).
[Crossref]

T. Inoue, M. D. Zoysa, T. Asano, S. Noda, “Filter-free nondispersive infrared sensing using narrow-bandwidth mid-infrared thermal emitters,” Appl. Phys. Express 7, 012103 (2014).
[Crossref]

T. Inoue, M. D. Zoysa, T. Asano, S. Noda, “Realization of dynamic thermal emission control,” Nat. Mater. 13, 928–931 (2014).
[Crossref]

C.-M. Wang, D.-Y. Feng, “Omnidirectional thermal emitter based on plasmonic nanoantenna arrays,” Opt. Express 22, 1313–1318 (2014).
[Crossref]

2013 (6)

T. Inoue, T. Asano, M. D. Zoysa, A. Oskooi, S. Noda, “Design of single-mode narrow-bandwidth thermal emitters for enhanced infrared light sources,” J. Opt. Soc. Am. B 30, 165–172 (2013).
[Crossref]

V. Rinnerbauer, Y. X. Yeng, W. R. Chan, J. J. Senkevich, J. D. Joannopoulos, M. Soljačić, I. Celanovic, “High-temperature stability and selective thermal emission of polycrystalline tantalum photonic crystals,” Opt. Express 21, 11482–11491 (2013).
[Crossref]

T. Inoue, M. D. Zoysa, T. Asano, S. Noda, “Single-peak narrow-bandwidth mid-infrared thermal emitters based on quantum wells and photonic crystals,” Appl. Phys. Lett. 102, 191110 (2013).
[Crossref]

S. Molesky, C. J. Dewalt, Z. Jacob, “High-temperature epsilon-near-zero and epsilon-near-pole metamaterial emitters for thermophotovoltaics,” Opt. Express 21, A98–A110 (2013).
[Crossref]

J. Hodgkinson, R. P. Tatam, “Optical gas sensing: a review,” Meas. Sci. Technol. 24, 012004 (2013).
[Crossref]

W. R. Chan, P. Bermel, R. C. N. Pilawa-Podgurski, C. H. Marton, K. F. Jenson, J. J. Senkevich, J. D. Joannopoulos, M. Soljačić, I. Celanovic, “Toward high-energy-density, high-efficiency, and moderate-temperature chip-scale thermophotovoltaics,” Proc. Natl. Acad. Sci. USA 110, 5309–5314 (2013).
[Crossref]

2012 (5)

C. Wu, B. Neuner, J. John, A. Milder, B. Zollars, S. Savoy, G. Shvets, “Metamaterial-based integrated plasmonic absorber/emitter for solar thermo-photovoltaic systems,” J. Opt. 14, 024005 (2012).
[Crossref]

C. M. Watts, X. Liu, W. J. Padilla, “Metamaterial electromagnetic wave absorbers,” Adv. Mater. 24, OP98–OP120 (2012).

O. Ilic, M. Jablan, J. D. Joannopoulos, I. Celanovic, M. Soljačić, “Overcoming the black body limit in plasmonic and graphene near-field thermophotovoltaic systems,” Opt. Express 20, A367–A384 (2012).
[Crossref]

Y. Guo, C. L. Cortes, S. Molesky, Z. Jacob, “Broadband super-Planckian thermal emission from hyperbolic metamaterials,” Appl. Phys. Lett. 101, 131106 (2012).
[Crossref]

M. D. Zoysa, T. Asano, K. Mochizuki, A. Oskooi, T. Inoue, S. Noda, “Conversion of broadband to narrowband thermal emission through energy recycling,” Nat. Photonics 6, 535–539 (2012).
[Crossref]

2011 (5)

M. Ghebrebrhan, P. Bermel, Y. X. Yeng, I. Celanovic, M. Soljačić, J. D. Joannopoulos, “Tailoring thermal emission via Q matching of photonic crystal resonances,” Phys. Rev. A 83, 033810 (2011).
[Crossref]

X. Liu, T. Tyler, T. Starr, A. F. Starr, N. M. Jokerst, W. J. Padilla, “Taming the blackbody with infrared metamaterials as selective thermal emitters,” Phys. Rev. Lett. 107, 045901 (2011).
[Crossref]

J. A. Mason, S. Smith, D. Wasserman, “Strong absorption and selective thermal emission from a midinfrared metamaterial,” Appl. Phys. Lett. 98, 241105 (2011).
[Crossref]

M. N. Abbas, C.-W. Cheng, Y.-C. Chang, M.-H. Shih, H.-H. Chen, S.-C. Lee, “Angle and polarization independent narrow-band thermal emitter made of metallic disk on SiO2,” Appl. Phys. Lett. 98, 121116 (2011).
[Crossref]

K. Aydin, V. E. Ferry, R. M. Briggs, H. A. Atwater, “Broadband polarization-independent resonant light absorption using ultrathin plasmonic super absorbers,” Nat. Commun. 2, 517 (2011).
[Crossref]

2010 (1)

X. Liu, T. Starr, A. F. Starr, W. J. Padilla, “Infrared spatial and frequency selective metamaterial with near-unity absorbance,” Phys. Rev. Lett. 104, 207403 (2010).
[Crossref]

2009 (4)

L. S. Rothman, I. E. Gordon, A. Barbe, D. C. Benner, P. F. Bernath, M. Birk, V. Boudon, L. R. Brown, A. Campargue, J.-P. Champion, K. Chance, L. H. Coudert, V. Dana, V. M. Devi, S. Fally, J.-M. Flaud, R. R. Gamache, A. Goldman, D. Jacquemart, I. Kleiner, N. Lacome, W. J. Lafferty, J.-Y. Mandin, S. T. Massie, S. N. Mikhailenko, C. E. Miller, N. Moazzen-Ahmadi, O. V. Naumenko, A. V. Nikitin, J. Orphal, V. I. Perevalov, A. Perrin, A. Predoi-Cross, C. P. Rinsland, M. Rotger, M. Simeckova, M. A. H. Smith, K. Sung, S. A. Tashkun, J. Tennyson, R. A. Toth, A. C. Vandaele, J. Vander Auwera, “The HITRAN 2008 molecular spectroscopic database,” J. Quant. Spectrosc. Radiat. Transfer 110, 533–572 (2009).
[Crossref]

S. Basu, Z. M. Zhang, C. J. Fu, “Review of near-field thermal radiation and its application to energy conversion,” Int. J. Energy Res. 33, 1203–1232 (2009).
[Crossref]

E. Rephaeli, S. Fan, “Absorber and emitter for solar thermo-photovoltaic systems to achieve efficiency exceeding the Shockley–Queisser limit,” Opt. Express 17, 15145–15159 (2009).
[Crossref]

T. Asano, K. Mochizuki, M. Yamaguchi, M. Chaminda, S. Noda, “Spectrally selective thermal radiation based on intersubband transitions and photonic crystals,” Opt. Express 17, 19190–19202 (2009).
[Crossref]

2008 (6)

L. Hu, A. Narayanaswamy, X. Chen, G. Chen, “Near-field thermal radiation between two closely spaced glass plates exceeding Planck’s blackbody radiation law,” Appl. Phys. Lett. 92, 133106 (2008).
[Crossref]

N. I. Landy, S. Sajuyigbe, J. J. Mock, D. R. Smith, W. J. Padilla, “Perfect metamaterial absorber,” Phys. Rev. Lett. 100, 207402 (2008).
[Crossref]

K. Ikeda, H. T. Miyazaki, T. Kasaya, K. Yamamoto, Y. Inoue, K. Fujimura, T. Kanakugi, M. Okada, K. Hatade, S. Kitagawa, “Controlled thermal emission of polarized infrared waves from arrayed plasmon nanocavities,” Appl. Phys. Lett. 92, 021117 (2008).
[Crossref]

H. T. Miyazaki, K. Ikeda, T. Kasaya, K. Yamamoto, Y. Inoue, K. Fujimura, T. Kanakugi, M. Okada, K. Hatade, S. Kitagawa, “Thermal emission of two-color polarized infrared waves from integrated plasmon cavities,” Appl. Phys. Lett. 92, 141114 (2008).
[Crossref]

G. Biener, N. Dahan, A. Niv, V. Kleiner, E. Hasman, “Highly coherent thermal emission obtained by plasmonic bandgap structures,” Appl. Phys. Lett. 92, 081913 (2008).
[Crossref]

I. Puscasu, W. L. Schaich, “Narrow-band, tunable infrared emission from arrays of microstrip patches,” Appl. Phys. Lett. 92, 233102 (2008).
[Crossref]

2007 (1)

R. Rubio, J. Santander, L. Fonseca, N. Sabaté, I. Gràcia, C. Cané, S. Udina, S. Marco, “Non-selective NDIR array for gas detection,” Sens. Actuators B 127, 69–73 (2007).
[Crossref]

2006 (2)

D. L. C. Chan, M. Soljačić, J. D. Joannopoulos, “Thermal emission and design in 2D-periodic metallic photonic crystal slabs,” Opt. Express 14, 8785–8796 (2006).
[Crossref]

D. L. C. Chan, I. Celanovic, J. D. Joannopoulos, M. Soljačić, “Emulating one-dimensional resonant Q-matching behavior in a two-dimensional system via Fano resonances,” Phys. Rev. A 74, 064901 (2006).
[Crossref]

2005 (2)

B. J. Lee, C. J. Fu, Z. M. Zhang, “Coherent thermal emission from one-dimensional photonic crystals,” Appl. Phys. Lett. 87, 071904 (2005).
[Crossref]

K. Joulain, J.-P. Mulet, F. Marquier, R. Carminati, J.-J. Greffet, “Surface electromagnetic waves thermally excited: Radiative heat transfer, coherence properties and Casimir forces revisited in the near field,” Surf. Sci. Rep. 57, 59–112 (2005).
[Crossref]

2004 (1)

H. Sai, H. Yugami, “Thermophotovoltaic generation with selective radiators based on tungsten surface gratings,” Appl. Phys. Lett. 85, 3399–3401 (2004).
[Crossref]

2003 (3)

S. Y. Lin, J. Moreno, J. G. Fleming, “Three-dimensional photonic-crystal emitter for thermal photovoltaic power generation,” Appl. Phys. Lett. 83, 380–382 (2003).
[Crossref]

F. Kusunoki, J. Takahara, T. Kobayasi, “Qualitative change of resonant peaks in thermal emission from periodic array of microcavities,” Electron. Lett. 39, 23–24 (2003).
[Crossref]

H. Sai, Y. Kanamori, H. Yugami, “High-temperature resistive surface grating for spectral control of thermal radiation,” Appl. Phys. Lett. 82, 1685–1687 (2003).
[Crossref]

2002 (6)

B. Bitnar, W. Durisch, J.-C. Mayor, H. Sigg, H. R. Tschudi, “Characterization of rare earth selective emitters for thermophotovoltaic applications,” Sol. Energy Mater. Sol. Cells 73, 221–234 (2002).
[Crossref]

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J. Meléndez, A. J. de Castro, F. López, J. Meneses, “Spectrally selective gas cell for electrooptical infrared compact multigas sensor,” Sens. Actuators A 47, 417–421 (1995).
[Crossref]

Sens. Actuators B (1)

R. Rubio, J. Santander, L. Fonseca, N. Sabaté, I. Gràcia, C. Cané, S. Udina, S. Marco, “Non-selective NDIR array for gas detection,” Sens. Actuators B 127, 69–73 (2007).
[Crossref]

Sol. Energy Mater. Sol. Cells (1)

B. Bitnar, W. Durisch, J.-C. Mayor, H. Sigg, H. R. Tschudi, “Characterization of rare earth selective emitters for thermophotovoltaic applications,” Sol. Energy Mater. Sol. Cells 73, 221–234 (2002).
[Crossref]

Surf. Sci. Rep. (1)

K. Joulain, J.-P. Mulet, F. Marquier, R. Carminati, J.-J. Greffet, “Surface electromagnetic waves thermally excited: Radiative heat transfer, coherence properties and Casimir forces revisited in the near field,” Surf. Sci. Rep. 57, 59–112 (2005).
[Crossref]

Other (2)

J. D. Joannopoulos, S. G. Johnson, R. D. Meade, J. N. Winn, Photonic Crystals: Molding the Flow of Light (Princeton University, 2008).

D. B. Brace, The Laws of Radiation and Absorption: Memoirs by Prévost, Stewart, Kirchhoff, and Kirchhoff and Bunsen (American Book Company, 1901).

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Figures (8)

Fig. 1.
Fig. 1.

(a) Schematic of a 2D array of rectangular metallic microcavities for thermal emission control. (b) Scanning electron micrograph (SEM) image of a fabricated emitter made of single crystalline W with Λ=1.0μm, a=0.8μm, and d=0.8μm. (c) Measured normal emissivity spectrum of the 2D array of microcavities and a flat W substrate at 1180 K. The solid line with circles represents a reported emissivity spectrum of flat W. (d) Thermal emission spectra of a polycrystalline Ta photonic crystal with HfO2 coating at different temperatures (solid lines), compared to the simulated emission of a Ta photonic crystal (dashed line), calculated emission of flat Ta (dashed-dotted line), and calculated blackbody emission (dashed black line) at 982°C. The inset shows a SEM image of the fabricated Ta photonic crystal. (a)–(c) reprinted from Ref. [21] with permission from AIP Publishing LLC (2003); (d) reprinted from Ref. [18], Copyright Optical Society of America (2013).

Fig. 2.
Fig. 2.

(a) SEM image of a fabricated Au/Cr grating. (b) Measured TM-polarized emission spectra from a grating with period of 2.99 μm, width of 316 nm, and depth of 1.04 μm. The thermal emission spectrum of the reference blackbody sample at 503 K is also shown. Reprinted from Ref. [22] with permission from AIP Publishing LLC (2008).

Fig. 3.
Fig. 3.

(a) Schematic of single-band (left) and dual-band (right) infrared metamaterial thermal emitters. (b) Measured emissivity spectra of fabricated single-band (left) and dual-band (right) metamaterial thermal emitters at five different temperatures. Reprinted from Ref. [26] with permission from American Physical Society (2011).

Fig. 4.
Fig. 4.

(a) Schematic of a multilayer metamaterial composed of alternating layers of metal and dielectric. (b) Calculated emissivity of a planar multilayer structure. The metamaterial is composed of 20 unit cells of 5 nm thick tantalum (modeled by a Drude relation) and 45 nm of titanium dioxide on optically thick tantalum substrate. The inset shows the effective medium parameters as functions of wavelength. Reprinted from Ref. [30] with permission from Optical Society of America (2012).

Fig. 5.
Fig. 5.

Measured (solid) and calculated (dashed) reflectivity spectra of a SiC grating at room temperature for different observation angles 30° (green) and 45° (red). The incident light is TM-polarized. Reprinted from Ref. [37] with permission from Macmillan Publishers Ltd: Nature (London) (2002).

Fig. 6.
Fig. 6.

(a) Schematic of ISB-Ts in multiple quantum wells used for control of thermal emission. (b) Thermal emission spectra of the quantum wells at 100°C for transverse-magnetic (TM) and transverse-electric (TE) polarization. The optical setup is shown schematically in the left panel, where θB denotes Brewster’s angle of GaAs. The dashed line shows the emission spectrum of a blackbody reference. Reprinted from Ref. [42].

Fig. 7.
Fig. 7.

(a) Structure of a single-peak, narrowband thermal emitter based on multiple quantum wells and a photonic crystal (PC) slab. The unit cell (marked in yellow) contains two rods with different radii. (b) Calculated photonic band diagram for the TM-like modes. The structural parameters for the calculation were set to a=7.0μm, h=2.6μm, t=0.6μm, r1=0.145a, and r2=0.135a. The position of the ISB-T absorption spectrum is shaded gray for reference. (c) Calculated Q factor of the Γ-point resonant mode in Fig. 7(b), determined by the intersubband absorption (Qabs) as a function of the number of quantum well layers. An ISB-T absorption coefficient of 4200cm1 at the transition wavelength was assumed in the calculation. (d) Calculated Q factor of the same mode, determined by the far-field radiation (Qrad), as a function of the ratio of the two rod radii (r2/r1). The inset shows the electric-field (Ex) distribution of the mode. (e) Measured thermal radiation intensity spectra of the fabricated emitter (a=7.6μm, h=1.3μm, t=0.6μm, r1=0.17a, r2=0.15a, and Nw=13) and reference blackbody sample in the surface-normal direction at a temperature of 200°C. Reprinted from Refs. [43] and [44].

Fig. 8.
Fig. 8.

Infrared camera image of the dynamically controllable narrowband thermal emitter (100°C) with and without reverse bias. When the reverse bias is applied, the electrons in the MQWs are extracted from the wells, leading to the decrease in the absorptivity (emissivity) of the device. Reprinted from Ref. [54].

Equations (2)

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ε=εMρ+εD(1ρ)ε=εMεDεM(1ρ)+εDρ,
εU(ω)=ξ1+ξ×1/QabsQrad(ω/ωres1)2+(1/2Qabs+1/2Qrad)2,

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