• Photonics Research
  • Vol. 3, Issue 6, 329 (2015)
Huacun Wang1、2, Qin Chen1、*, Long Wen1, Shichao Song1, Xin Hu1, and Gaiqi Xu1
Author Affiliations
  • 1Key Laboratory of Nanodevices and Applications-CAS and Collaborative Innovation Center of Suzhou Nano Science and Technology, Suzhou Institute of Nano-Tech and Nano-Bionics, Chinese Academy of Sciences (CAS), Suzhou 215123, China
  • 2Department of Electronic Information Materials, Shanghai Leading Academic Disciplines, Shanghai University, Shanghai 200072, China
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    DOI: 10.1364/PRJ.3.000329 Cite this Article Set citation alerts
    Huacun Wang, Qin Chen, Long Wen, Shichao Song, Xin Hu, Gaiqi Xu. Titanium-nitride-based integrated plasmonic absorber/ emitter for solar thermophotovoltaic application[J]. Photonics Research, 2015, 3(6): 329 Copy Citation Text show less
    Schematic of the BANE structure and the geometric parameters of one unit cell. The BANE film is a three-layered structure consisting of lossy TiN cross features on top of a lossless AlN layer and a substrate of TiN.
    Fig. 1. Schematic of the BANE structure and the geometric parameters of one unit cell. The BANE film is a three-layered structure consisting of lossy TiN cross features on top of a lossless AlN layer and a substrate of TiN.
    (a) Polarization-averaged normalized absorption spectra of a BANE structure: L=0.28 μm; W=0.11 μm; P=0.4 μm; H1=0.08 μm; H2=0.03 μm; H3=0.1 μm for various incidence angles. (b) Radiation spectra of blackbody and the BANE structure at 800, 1500, and 2000 K. (c) Normalized absorption spectra for varying L of 0.24, 0.26, 0.28, 0.3, and 0.32 μm. Normalized absorption spectrum as a function of width of cross structure (W in Fig. 1) in (d) and height of cross structure (H1 in Fig. 1) in (e). (f) Normalized reflection (black line) transmission (red line) and absorption (blue line) spectra of 0.1 μm TiN film.
    Fig. 2. (a) Polarization-averaged normalized absorption spectra of a BANE structure: L=0.28μm; W=0.11μm; P=0.4μm; H1=0.08μm; H2=0.03μm; H3=0.1μm for various incidence angles. (b) Radiation spectra of blackbody and the BANE structure at 800, 1500, and 2000 K. (c) Normalized absorption spectra for varying L of 0.24, 0.26, 0.28, 0.3, and 0.32 μm. Normalized absorption spectrum as a function of width of cross structure (W in Fig. 1) in (d) and height of cross structure (H1 in Fig. 1) in (e). (f) Normalized reflection (black line) transmission (red line) and absorption (blue line) spectra of 0.1 μm TiN film.
    (a) Field distributions. (b) Resonance wavelength of 2 μm. (c), (d) Nonresonance wavelength of 1.25 μm for the BANE structure in Fig. 2(a) at normal incidence. (a) and (c) Electric field. (b) and (d) Magnetic field.
    Fig. 3. (a) Field distributions. (b) Resonance wavelength of 2 μm. (c), (d) Nonresonance wavelength of 1.25 μm for the BANE structure in Fig. 2(a) at normal incidence. (a) and (c) Electric field. (b) and (d) Magnetic field.
    (a) Artificial absorption/emission spectrum ϵart(λ). (b) Maximum overall PCE as a function of bw1 and bw3.
    Fig. 4. (a) Artificial absorption/emission spectrum ϵart(λ). (b) Maximum overall PCE as a function of bw1 and bw3.
    Contours of (a) ultimate efficiency, U, (b) recombination efficiency, ν, (c) impedance matching factor, m, (d) overall STPV efficiency, η.
    Fig. 5. Contours of (a) ultimate efficiency, U, (b) recombination efficiency, ν, (c) impedance matching factor, m, (d) overall STPV efficiency, η.
    Huacun Wang, Qin Chen, Long Wen, Shichao Song, Xin Hu, Gaiqi Xu. Titanium-nitride-based integrated plasmonic absorber/ emitter for solar thermophotovoltaic application[J]. Photonics Research, 2015, 3(6): 329
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