Abstract

The reflection and emission properties of an infrared emitter, which is a plasmonic multilayer structure consisting of a relief metallic grating, a waveguide layer, and a metallic substrate are investigated both experimentally and theoretically. A localized surface plasmon polariton (SPP) mode which is angular-independent in almost the full range of incident angles is observed. The thermal emission of this structure is also measured. It is found that the emission peak coincides with the angular-independent localized SPP mode. In addition, the emission spectrum of the plasmonic emitter can be predicted by investigating the reflectance spectrum.

©2007 Optical Society of America

1. Introduction

Textured metallic structure with a subwavelength scale is known to strongly modify the electromagnetic response. This remarkable feature has potential in applications in both passive and active optical devices. In passive optical devices, a metallic film patterned with periodic subwavelength hole arrays can exhibit extraordinary optical transmission [1] which can be used in photolithography and near-field microscopy [2–4]. In active optical devices, the surface plasmon polaritons (SPPs), which play a crucial role in light-matter interactions, were proposed to modify the emission properties of a nearby active emission layer [5] and lead to more efficient light emitting devices [6]. Moreover, a dielectric cavity sandwiched between a perforated metal film and a flat metallic film has strong coupling effects via evanescent fields [7, 8]. The coupling interaction strongly depends on the thickness of the metal film [9]. When the thickness of the metal film is small, the coupling interaction is strong, and new SPP modes can be formed. Through tuning the coupling of the SPP modes, versatile plasmonic infrared (IR) emitters were made [10, 11]. This kind of the IR emitter with narrow bandwidth emission property is very useful in the studies of the reaction of biological systems, environmental protection, and industrial environment [12–18].

2. Device descriptions and fabrications

In this Letter we study the reflection properties of a plasmonic multilayer structure which consists of a relief metallic grating, a waveguide layer, and a metallic substrate as depicted in Fig. 1. This plasmonic multilayer structure can also be used as an IR emitter. The relations of the reflection and emission properties were investigated in details. The grating periodicity is denoted by Λ, the filling factor is f, the depth is denoted by tg, and its complex dielectric constant is denoted by εm where εmmr+mi. Between and above the grating grooves the dielectric constant is denoted by εAir. The thickness of the SiO2 waveguide layer is assumed to be tw and its dielectric constant is denoted by εw. The material of the metallic substrate is identical to the grating, εm. The substrate thickness is assumed to be infinite. The structure is illuminated with an incident plane wave at an angle θi. The input light is TM-polarized in which the magnetic vector is parallel to the grating grooves (i.e., parallel to the y-axis). The wavelength-dependent optical constants of the investigated materials are taken from ref. [19].

 figure: Fig. 1.

Fig. 1. Basic geometry of an IR emitter considered. It is a plasmonic multilayer structure consisting of a relief metallic grating, a waveguide layer, and a metallic substrate.

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The fabrication processes of the plasmonic multilayer structure are described as follows. An optically thick Ag metal film was deposited on the front side of a Si substrate followed by a SiO2 layer deposited with the electron beam evaporator. Then, a grating structure of 100nm thick silver film was patterned onto the SiO2 layer by deposition and lifted-off techniques. The geometric parameters of the fabricated system are as follows: Λ=3000nm, =1800nm, tg=100nm and tw=23nm. The reflectance spectrum of the device was measured by a Perkin Elmer 2000 Fourier transform infrared spectrometer (FTIR) system with a wave number resolution of 8 cm−1.

3. Angular-dependent reflectance spectra of the plasmonic multilayer filter

Figures 2(a) and 2(b) shows the measured and simulated angle-dependent reflectance spectra. Darker shading represents lower reflectivity. Because of the limitation of the FTIR system, we can only measure the reflectance spectrum with unpolarized light with an incident angle from 12° to 65°. The TM-polarized spectrum was simulated by the Rigorous Coupled Wave Analysis (RCWA) method [20]. The simulation parameters of the plasmonic multilayer structure used to give a best fit are: Λ=3000nm, =1900nm, tg=100nm and tw=25nm. For normal incidence, there were three resonance dips occurring at 0.17eV, 0.38eV and 0.41eV. As the incident angle increases, the resonant dip at 0.41eV splits into two dips. At the same time, the resonant dips at 0.17eV and 0.38eV are independent of the incident angle. The simulated pattern agrees well with the experiment.

 figure: Fig. 2.

Fig. 2. Angle-dependent reflectance spectra of the IR emitter. (a) measured. (b) RCWA simulation. The geometric parameters used in the simulation were: Λ=3000nm, =1900nm, tg=100nm and tw=25nm.

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First, we discuss the resonant dip at 0.41eV for normal incidence. This dip corresponds to the grating-coupled SPPs. Typically, the dispersion curves reveal the resonances due to the excitation of SPPs at either the SiO2/Ag (SA) or Air/Ag (AA) interfaces of the metal film. The resonant dip of the dispersion is denoted according to the conservation of momentum for SPPs: kSPP=kx+G, where kSPP is the wave vector of SPPs; G=2πm/Λ denotes the reciprocal lattice vectors of the grating; m is an integer. The simulated dispersion reveals the grating-coupled SPP AA (AA[+1], AA[-1] and AA[-2]) modes with sharp resonant features. In our measurements, the contrast of the grating coupled modes are low owing to that the probe beam is a converging beam with a numerical aperture (NA) smaller than 0.2.

When the structure is an Ag grating on a SiO2 substrate with infinite thickness, the field strength of the SPP decays exponentially away from the SA interface, as shown by the dotted line in Fig. 1. On the other hands, when the lower part of the SiO2 substrate is replaced by a flat Ag layer, leaving an SiO2 slab between the Ag grating and the Ag substrate, the SPP modes localized at the top and bottom of the SiO2 slab become coupled. At this time, the field distribution at the sandwiched SiO2 layer can be seen as a linear combination of two exponentially decaying SPPs of the two SA interfaces. Therefore, new SPP modes can be formed within the Ag/SiO2/Ag (ASA) interface. Except the grating-coupled modes, there were some additional resonant reflection dips shown in Fig. 2. These resonant dips show very little angular dispersion. Especially for the dip at 0.17eV, which is angular-independent for almost the entire range of incident angles. The dips at 0.27eV and 0.5eV exist for a larger incident angle while the dip at 0.38eV exists for a small incident angle. This angular-independent behavior implies that the group velocity in x-direction, ∂ω/∂kx is zero. This is because that the SPP modes, which are localized SPP (LSPP) modes, also have a standing wave character in the x-direction as we shall illustrate below.

To understand the nature of these resonances, it is instructive to investigate their field distributions. As shown in Fig. 2, there were four resonant reflection dips, respectively located at 0.17eV, 0.27eV, 0.38eV and 0.5eV, which were almost independent of the incident angle. The resonant dips display different resonant behaviors versus the incident angle. Fig. 3(a) shows the Hy 2 distribution along the x-axis at the grating/SiO2 interface for the four LSPP modes at 0.17eV, 0.27eV, 0.38eV and 0.5eV, respectively. From the nodal structures, we can identify them as the n=1, n=2, n=3 and n=4 Fabry-Perot cavity modes, respectively. Fig. 3(b) shows the Hy 2 distribution (averaged over the period in x) along the z-axis under the Ag ridge of the grating for the four LSPP modes. The dips at 0.17eV (square) and 0.38eV (triangle) are calculated for an incident angle of 0° while the dips at 0.27eV (circular) and 0.5eV (star) are calculated for an incident angle of 89°. From Fig. 3(b), it can be seen that the LSPP modes were resonant along lateral direction under the Ag ridge with an effective cavity length of β(λ)Λf/k 0, where β(λ) is a wavelength dependent propagation constant. For a deceasing tw/λ, β(λ) is increasing. The field strength decays exponentially first and then grows exponentially for 0nm< z <100nm. In the waveguide region (100nm< z <125nm), the field strength is enhanced significantly for the 0.17eV mode. In the Ag substrate region, the field strength exponentially decays again, as it should.

 figure: Fig. 3.

Fig. 3. Magnetic field strength, Hy 2, (a) along the x-axis at the center of the Ag ridge (b) along the z-axis at the grating/SiO2 interface. The dips at 0.17eV (square) and 0.38eV (triangle) are calculated for an incident angle of 0o while the dips at 0.27eV (circular) and 0.5eV (star) are calculated for an incident angle of 89°. The geometric parameters were: Λ=3000nm, =1900nm, tg=100nm and tw=25nm.

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4. Thermal radiation of the IR emitter

Finally, the thermal radiation of the plasmonic multilayer structure was measured by heating the sample with a DC current in a chamber with a pressure of 3 mTorr. The device area is 1×1cm2. The structure is a SiO2 cavity sandwiched between a one-dimensional relief metallic grating and a flat metallic film. The thermal radiation was collected by a 45° off-axis concave mirror with a NA of 0.1 and then reflected into the FTIR system. The solid lines shown in Fig. 4 were the measured thermal emission spectrum of the IR emitter which was heated up to 220°C (red line) and 260°C (black line), respectively. The spectra show a sharp emission peak at 7.2μm which was very different from a typical blackbody emission spectrum. Nevertheless, the emission spectrum can be predicted by investigating the angular-dependent reflectance spectrum. For the case that λ>>Λ, the absorptivity of the device is (1-reflectance). According to the Kirchhoff’s law [21], the emissivity is equal to absorptivity. Therefore, the emission spectrum of the plasmonic structure can be predicted by multiplying the inherent thermal radiation profile and the angular-dependent absorptivity[22]:

Emission(λ)=TR(λ)(10π2R(λ,θ)cos(θ))

where R(λ,θ) is the reflectance of the proposed structure at an incident angle, θ. In this paper, TR(λ) is taken to be the thermal radiation curve without the grating structure. Previously, Kreiter et al. also performed emission measurements related to surface plasmons on a grating.[23] Other related works can be found in Refs. [24–26]. Using the simulated R(λ,θ), the emission spectrum can be calculated from Eq. (1). Here, R(λ,θ) has been shown in Fig. 2(b). The dashed lines shown in Fig. 4 are the simulated thermal radiation spectrum of the IR emitter which was heated up to 220°C (red line) and 260°C (black line), respectively. The simulated results show a fair agreement with the measurement. However, the sideband of the measured radiation spectrum was higher than the simulated one. This sideband might come from the heating plate. Furthermore, the dielectric function of the materials involved could also change at high temperature, which would lead to discrepancies between theory and experiment. Comparing to Fig. 2(b), the emission peak coincides with the angular-independent reflection dip which corresponds to an LSPP mode mentioned above. It is worth mentioning that the thermal emission light inside the SiO2 cavity suffers from the total internal reflection (TIR) for a grating-less case. However, for our proposed structure, the emitted light is coupled into the LSPP mode and then re-radiates into the free-space. At this time, the emission efficiency is not limited by the TIR. This implies that an angular independent localized SPP mode can lead to an enhanced emission peak.

 figure: Fig. 4.

Fig. 4. (a) Simulated (dashed line) and measured (solid line) emission spectrum of the IR emitter for 220°C (red line) and 260°C (black line), respectively. The geometric parameters were: Λ=3000nm, =1900nm, tg=100nm and tw=25nm.

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5. Conclusion

In summery, the reflection and emission properties of an IR emitter, which is a plasmonic multilayer structure consisting of a relief metallic grating, a waveguide layer, and a metallic substrate, are investigated both experimentally and theoretically. The resonant grating-coupled and localized SPP modes are identified. An LSPP mode, which is angular-independent in almost the full range of incident angles is observed. The relations of the reflection and emission properties are investigated in details. The emission peak coincides with the angular-independent reflection dip simulated by the RCWA method. The thermal radiation spectrum of the structure can be predicted by investigating the reflectance properties. We demonstrate that this method is useful for the design of an effective LED light extraction structure.

Acknowledgment

This work was supported by Academia Sinica, Taiwan.

References and Links

1. T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through subwavelength hole arrays,” Nature 391, 667–669 (1998) [CrossRef]  

2. X. Luo and T. Ishihara, “Surface plasmon resonant interference nanolithography technique,” Appl. Phys. Lett. 84, 4780–4782 (2004) [CrossRef]  

3. L. Salomon, F. Grillot, A. V. Zayats, and F. de Fornel, “Near-Field Distribution of Optical Transmission of Periodic Subwavelength Holes in a Metal Film,” Phys. Rev. Lett. 86, 1110–1113 (2001). [CrossRef]   [PubMed]  

4. J. Hashizume and F. Koyama, “Plasmon Enhanced Optical Near-field Probing of Metal Nanoaperture Surface Emitting Laser,” Opt. Express. 12, 6391–6396 (2004). [CrossRef]   [PubMed]  

5. W. L. Barnes, “Fluorescence near interfaces: the role of photonic mode density,” J. Mod. Opt. 45, 661–699 (1998). [CrossRef]  

6. K. Okamoto, I. Niki, A. Shvartser, Y. Narukawa, T. Mukai, and A. Scherer, “Surface-plasmon-enhanced light emitters based on InGaN quantum wells,” Nat. Mater. 3, 601–605 (2004). [CrossRef]   [PubMed]  

7. S. A. Darmanyan and A. V. Zayats, “Light tunneling via resonant surface plasmon polariton states and the enhanced transmission of periodically nanostructured metal films: An analytical study,” Phys. Rev. B 67, 035424-1-7 (2003). [CrossRef]  

8. L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001). [CrossRef]   [PubMed]  

9. A. Christ, T. Zentgraf, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Controlling the interaction between localized and delocalized surface plasmon modes: Experiment and numerical calculations,” Phys. Rev. B. 74, 155435-1-8 (2006). [CrossRef]  

10. M. W. Tsai, T. H. Chuang, C. Y. Meng, Y. T. Chang, and S. C. Lee, “High performance midinfrared narrow-band plasmonic thermal emitter,” App. Phys. Lett. 89, 173116–173118 (2006). [CrossRef]  

11. T. H. Chuang, M. W. Tsai, Y. T. Chang, and S. C. Lee, “Remotely coupled surface plasmons in a two-colored plasmonic thermal emitter,” App. Phys. Lett. 89, 173128–173130 (2006). [CrossRef]  

12. M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002). [CrossRef]  

13. I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003). [CrossRef]  

14. I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005). [CrossRef]  

15. S. Y. Lin, J. Moreno, and J. G. Fleming, “A 3D Photonic-Crystal Emitter for Thermal Photovoltaic Generation,” Appl. Phys. Lett. 83, 380–382 (2003). [CrossRef]  

16. S. Y. Lin, J. G. Fleming, and I. El-Kady, “Experimental observation of photonic-crystal emission near a photonic band edge,” Appl. Phys. Lett. 83, 593–595 (2003). [CrossRef]  

17. P. Ben-Abdallah and B. Ni, “Single-defect Bragg stacks for high-power narrow-band thermal emission,” J. Appl. Phys. 97, 104910-1-5 (2005). [CrossRef]  

18. I. Celanovic, D. Perreault, and J. Kassakian, “Resonant-cavity enhanced thermal emission,” Phys. Rev. B 72, 075127-1-6 (2005). [CrossRef]  

19. E. D. Palik, Handbook of Optical Constants of Solids (Academic Press, Boston, 1985).

20. M.G. Moharam, E.B. Grann, D.A. Pommet, and T. K. Gaylord, “Formulation for stable and efficient implementation of the rigorous coupled-wave analysis of binary gratings,” J. Opt. Soc. Am. A 12, 1068–1076 (1995); “Stable implementation of the rigorous coupled-wave analysis of surface-relief gratings: enhance transmittance matrix approach,” J. Opt. Soc. Am. A 12, 1077–1086 (1995). [CrossRef]  

21. J. J. Greffet and M. Nieto-Vesperinas, “Field theory for generalized bidirectional reflectivity: derivation of Helmholtz’s reciprocity principle and Kirchhoff’s law“, J. Opt. Soc. Am. A 15, 2735–2744 (1998). [CrossRef]  

22. R. Siegel and J. Howell, Thermal Radiation Heat Transfer (New York: Hemisphere Publishing Corporation, 1981).

23. M. Kreiter, J. Oster, R. Sambles, S. Herminghaus, S. Mittler-Neher, and W. Knoll, “Thermally induced emission of light from a metallic diffraction grating, mediated by surface plasmons,” Opt. Commun. 168, 117–122 (1999) [CrossRef]  

24. J.J. Greffet, R. Carminati, K. Joulain, J.P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature , 416, 61–64 (2002). [CrossRef]   [PubMed]  

25. F. Marquier, K. Joulain, J.P. Mulet, R. Carminati, J.J. Greffet, and Y. Chen, “Coherent spontaneous emission of light by thermal sources,” Phys. Rev. B 69, 155412-1-11 (2004). [CrossRef]  

26. M. Laroche, C. Arnold, F. Marquier, R. Carminati, J. J. Greffet, S. Collin, N. Bardou, and J. L. Pelouard, “Highly directional radiation generated by a tungsten thermal source,” Opt. Lett. 30, 2623–2625 (2005). [CrossRef]   [PubMed]  

References

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  • |

  1. T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through subwavelength hole arrays,” Nature 391, 667–669 (1998)
    [Crossref]
  2. X. Luo and T. Ishihara, “Surface plasmon resonant interference nanolithography technique,” Appl. Phys. Lett. 84, 4780–4782 (2004)
    [Crossref]
  3. L. Salomon, F. Grillot, A. V. Zayats, and F. de Fornel, “Near-Field Distribution of Optical Transmission of Periodic Subwavelength Holes in a Metal Film,” Phys. Rev. Lett. 86, 1110–1113 (2001).
    [Crossref] [PubMed]
  4. J. Hashizume and F. Koyama, “Plasmon Enhanced Optical Near-field Probing of Metal Nanoaperture Surface Emitting Laser,” Opt. Express. 12, 6391–6396 (2004).
    [Crossref] [PubMed]
  5. W. L. Barnes, “Fluorescence near interfaces: the role of photonic mode density,” J. Mod. Opt. 45, 661–699 (1998).
    [Crossref]
  6. K. Okamoto, I. Niki, A. Shvartser, Y. Narukawa, T. Mukai, and A. Scherer, “Surface-plasmon-enhanced light emitters based on InGaN quantum wells,” Nat. Mater. 3, 601–605 (2004).
    [Crossref] [PubMed]
  7. S. A. Darmanyan and A. V. Zayats, “Light tunneling via resonant surface plasmon polariton states and the enhanced transmission of periodically nanostructured metal films: An analytical study,” Phys. Rev. B 67, 035424-1-7 (2003).
    [Crossref]
  8. L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001).
    [Crossref] [PubMed]
  9. A. Christ, T. Zentgraf, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Controlling the interaction between localized and delocalized surface plasmon modes: Experiment and numerical calculations,” Phys. Rev. B. 74, 155435-1-8 (2006).
    [Crossref]
  10. M. W. Tsai, T. H. Chuang, C. Y. Meng, Y. T. Chang, and S. C. Lee, “High performance midinfrared narrow-band plasmonic thermal emitter,” App. Phys. Lett. 89, 173116–173118 (2006).
    [Crossref]
  11. T. H. Chuang, M. W. Tsai, Y. T. Chang, and S. C. Lee, “Remotely coupled surface plasmons in a two-colored plasmonic thermal emitter,” App. Phys. Lett. 89, 173128–173130 (2006).
    [Crossref]
  12. M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
    [Crossref]
  13. I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
    [Crossref]
  14. I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
    [Crossref]
  15. S. Y. Lin, J. Moreno, and J. G. Fleming, “A 3D Photonic-Crystal Emitter for Thermal Photovoltaic Generation,” Appl. Phys. Lett. 83, 380–382 (2003).
    [Crossref]
  16. S. Y. Lin, J. G. Fleming, and I. El-Kady, “Experimental observation of photonic-crystal emission near a photonic band edge,” Appl. Phys. Lett. 83, 593–595 (2003).
    [Crossref]
  17. P. Ben-Abdallah and B. Ni, “Single-defect Bragg stacks for high-power narrow-band thermal emission,” J. Appl. Phys. 97, 104910-1-5 (2005).
    [Crossref]
  18. I. Celanovic, D. Perreault, and J. Kassakian, “Resonant-cavity enhanced thermal emission,” Phys. Rev. B 72, 075127-1-6 (2005).
    [Crossref]
  19. E. D. Palik, Handbook of Optical Constants of Solids (Academic Press, Boston, 1985).
  20. M.G. Moharam, E.B. Grann, D.A. Pommet, and T. K. Gaylord, “Formulation for stable and efficient implementation of the rigorous coupled-wave analysis of binary gratings,” J. Opt. Soc. Am. A 12, 1068–1076 (1995); “Stable implementation of the rigorous coupled-wave analysis of surface-relief gratings: enhance transmittance matrix approach,” J. Opt. Soc. Am. A 12, 1077–1086 (1995).
    [Crossref]
  21. J. J. Greffet and M. Nieto-Vesperinas, “Field theory for generalized bidirectional reflectivity: derivation of Helmholtz’s reciprocity principle and Kirchhoff’s law“, J. Opt. Soc. Am. A 15, 2735–2744 (1998).
    [Crossref]
  22. R. Siegel and J. Howell, Thermal Radiation Heat Transfer (New York: Hemisphere Publishing Corporation, 1981).
  23. M. Kreiter, J. Oster, R. Sambles, S. Herminghaus, S. Mittler-Neher, and W. Knoll, “Thermally induced emission of light from a metallic diffraction grating, mediated by surface plasmons,” Opt. Commun. 168, 117–122 (1999)
    [Crossref]
  24. J.J. Greffet, R. Carminati, K. Joulain, J.P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature,  416, 61–64 (2002).
    [Crossref] [PubMed]
  25. F. Marquier, K. Joulain, J.P. Mulet, R. Carminati, J.J. Greffet, and Y. Chen, “Coherent spontaneous emission of light by thermal sources,” Phys. Rev. B 69, 155412-1-11 (2004).
    [Crossref]
  26. M. Laroche, C. Arnold, F. Marquier, R. Carminati, J. J. Greffet, S. Collin, N. Bardou, and J. L. Pelouard, “Highly directional radiation generated by a tungsten thermal source,” Opt. Lett. 30, 2623–2625 (2005).
    [Crossref] [PubMed]

2006 (3)

A. Christ, T. Zentgraf, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Controlling the interaction between localized and delocalized surface plasmon modes: Experiment and numerical calculations,” Phys. Rev. B. 74, 155435-1-8 (2006).
[Crossref]

M. W. Tsai, T. H. Chuang, C. Y. Meng, Y. T. Chang, and S. C. Lee, “High performance midinfrared narrow-band plasmonic thermal emitter,” App. Phys. Lett. 89, 173116–173118 (2006).
[Crossref]

T. H. Chuang, M. W. Tsai, Y. T. Chang, and S. C. Lee, “Remotely coupled surface plasmons in a two-colored plasmonic thermal emitter,” App. Phys. Lett. 89, 173128–173130 (2006).
[Crossref]

2005 (4)

I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
[Crossref]

P. Ben-Abdallah and B. Ni, “Single-defect Bragg stacks for high-power narrow-band thermal emission,” J. Appl. Phys. 97, 104910-1-5 (2005).
[Crossref]

I. Celanovic, D. Perreault, and J. Kassakian, “Resonant-cavity enhanced thermal emission,” Phys. Rev. B 72, 075127-1-6 (2005).
[Crossref]

M. Laroche, C. Arnold, F. Marquier, R. Carminati, J. J. Greffet, S. Collin, N. Bardou, and J. L. Pelouard, “Highly directional radiation generated by a tungsten thermal source,” Opt. Lett. 30, 2623–2625 (2005).
[Crossref] [PubMed]

2004 (4)

F. Marquier, K. Joulain, J.P. Mulet, R. Carminati, J.J. Greffet, and Y. Chen, “Coherent spontaneous emission of light by thermal sources,” Phys. Rev. B 69, 155412-1-11 (2004).
[Crossref]

K. Okamoto, I. Niki, A. Shvartser, Y. Narukawa, T. Mukai, and A. Scherer, “Surface-plasmon-enhanced light emitters based on InGaN quantum wells,” Nat. Mater. 3, 601–605 (2004).
[Crossref] [PubMed]

X. Luo and T. Ishihara, “Surface plasmon resonant interference nanolithography technique,” Appl. Phys. Lett. 84, 4780–4782 (2004)
[Crossref]

J. Hashizume and F. Koyama, “Plasmon Enhanced Optical Near-field Probing of Metal Nanoaperture Surface Emitting Laser,” Opt. Express. 12, 6391–6396 (2004).
[Crossref] [PubMed]

2003 (4)

S. A. Darmanyan and A. V. Zayats, “Light tunneling via resonant surface plasmon polariton states and the enhanced transmission of periodically nanostructured metal films: An analytical study,” Phys. Rev. B 67, 035424-1-7 (2003).
[Crossref]

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

S. Y. Lin, J. Moreno, and J. G. Fleming, “A 3D Photonic-Crystal Emitter for Thermal Photovoltaic Generation,” Appl. Phys. Lett. 83, 380–382 (2003).
[Crossref]

S. Y. Lin, J. G. Fleming, and I. El-Kady, “Experimental observation of photonic-crystal emission near a photonic band edge,” Appl. Phys. Lett. 83, 593–595 (2003).
[Crossref]

2002 (2)

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

J.J. Greffet, R. Carminati, K. Joulain, J.P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature,  416, 61–64 (2002).
[Crossref] [PubMed]

2001 (2)

L. Salomon, F. Grillot, A. V. Zayats, and F. de Fornel, “Near-Field Distribution of Optical Transmission of Periodic Subwavelength Holes in a Metal Film,” Phys. Rev. Lett. 86, 1110–1113 (2001).
[Crossref] [PubMed]

L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001).
[Crossref] [PubMed]

1999 (1)

M. Kreiter, J. Oster, R. Sambles, S. Herminghaus, S. Mittler-Neher, and W. Knoll, “Thermally induced emission of light from a metallic diffraction grating, mediated by surface plasmons,” Opt. Commun. 168, 117–122 (1999)
[Crossref]

1998 (3)

J. J. Greffet and M. Nieto-Vesperinas, “Field theory for generalized bidirectional reflectivity: derivation of Helmholtz’s reciprocity principle and Kirchhoff’s law“, J. Opt. Soc. Am. A 15, 2735–2744 (1998).
[Crossref]

T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through subwavelength hole arrays,” Nature 391, 667–669 (1998)
[Crossref]

W. L. Barnes, “Fluorescence near interfaces: the role of photonic mode density,” J. Mod. Opt. 45, 661–699 (1998).
[Crossref]

1995 (1)

Arnold, C.

Bardou, N.

Barnes, W. L.

W. L. Barnes, “Fluorescence near interfaces: the role of photonic mode density,” J. Mod. Opt. 45, 661–699 (1998).
[Crossref]

Ben-Abdallah, P.

P. Ben-Abdallah and B. Ni, “Single-defect Bragg stacks for high-power narrow-band thermal emission,” J. Appl. Phys. 97, 104910-1-5 (2005).
[Crossref]

Biswas, R.

I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
[Crossref]

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Carminati, R.

M. Laroche, C. Arnold, F. Marquier, R. Carminati, J. J. Greffet, S. Collin, N. Bardou, and J. L. Pelouard, “Highly directional radiation generated by a tungsten thermal source,” Opt. Lett. 30, 2623–2625 (2005).
[Crossref] [PubMed]

F. Marquier, K. Joulain, J.P. Mulet, R. Carminati, J.J. Greffet, and Y. Chen, “Coherent spontaneous emission of light by thermal sources,” Phys. Rev. B 69, 155412-1-11 (2004).
[Crossref]

J.J. Greffet, R. Carminati, K. Joulain, J.P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature,  416, 61–64 (2002).
[Crossref] [PubMed]

Celanovic, I.

I. Celanovic, D. Perreault, and J. Kassakian, “Resonant-cavity enhanced thermal emission,” Phys. Rev. B 72, 075127-1-6 (2005).
[Crossref]

Chang, Y. T.

M. W. Tsai, T. H. Chuang, C. Y. Meng, Y. T. Chang, and S. C. Lee, “High performance midinfrared narrow-band plasmonic thermal emitter,” App. Phys. Lett. 89, 173116–173118 (2006).
[Crossref]

T. H. Chuang, M. W. Tsai, Y. T. Chang, and S. C. Lee, “Remotely coupled surface plasmons in a two-colored plasmonic thermal emitter,” App. Phys. Lett. 89, 173128–173130 (2006).
[Crossref]

Chen, Y.

F. Marquier, K. Joulain, J.P. Mulet, R. Carminati, J.J. Greffet, and Y. Chen, “Coherent spontaneous emission of light by thermal sources,” Phys. Rev. B 69, 155412-1-11 (2004).
[Crossref]

J.J. Greffet, R. Carminati, K. Joulain, J.P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature,  416, 61–64 (2002).
[Crossref] [PubMed]

Choi, D. S.

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Christ, A.

A. Christ, T. Zentgraf, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Controlling the interaction between localized and delocalized surface plasmon modes: Experiment and numerical calculations,” Phys. Rev. B. 74, 155435-1-8 (2006).
[Crossref]

Chuang, T. H.

T. H. Chuang, M. W. Tsai, Y. T. Chang, and S. C. Lee, “Remotely coupled surface plasmons in a two-colored plasmonic thermal emitter,” App. Phys. Lett. 89, 173128–173130 (2006).
[Crossref]

M. W. Tsai, T. H. Chuang, C. Y. Meng, Y. T. Chang, and S. C. Lee, “High performance midinfrared narrow-band plasmonic thermal emitter,” App. Phys. Lett. 89, 173116–173118 (2006).
[Crossref]

Collin, S.

Daly, J.

I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
[Crossref]

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

Daly, J. T.

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Darmanyan, S. A.

S. A. Darmanyan and A. V. Zayats, “Light tunneling via resonant surface plasmon polariton states and the enhanced transmission of periodically nanostructured metal films: An analytical study,” Phys. Rev. B 67, 035424-1-7 (2003).
[Crossref]

de Fornel, F.

L. Salomon, F. Grillot, A. V. Zayats, and F. de Fornel, “Near-Field Distribution of Optical Transmission of Periodic Subwavelength Holes in a Metal Film,” Phys. Rev. Lett. 86, 1110–1113 (2001).
[Crossref] [PubMed]

Ding, C. G.

I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
[Crossref]

Ebbesen, T. W.

L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001).
[Crossref] [PubMed]

T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through subwavelength hole arrays,” Nature 391, 667–669 (1998)
[Crossref]

El-Kady, I.

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

S. Y. Lin, J. G. Fleming, and I. El-Kady, “Experimental observation of photonic-crystal emission near a photonic band edge,” Appl. Phys. Lett. 83, 593–595 (2003).
[Crossref]

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Fleming, J. G.

S. Y. Lin, J. Moreno, and J. G. Fleming, “A 3D Photonic-Crystal Emitter for Thermal Photovoltaic Generation,” Appl. Phys. Lett. 83, 380–382 (2003).
[Crossref]

S. Y. Lin, J. G. Fleming, and I. El-Kady, “Experimental observation of photonic-crystal emission near a photonic band edge,” Appl. Phys. Lett. 83, 593–595 (2003).
[Crossref]

Garcia-Vidal, F. J.

L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001).
[Crossref] [PubMed]

Gaylord, T. K.

George, T.

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Ghaemi, H. F.

T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through subwavelength hole arrays,” Nature 391, 667–669 (1998)
[Crossref]

Giessen, H.

A. Christ, T. Zentgraf, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Controlling the interaction between localized and delocalized surface plasmon modes: Experiment and numerical calculations,” Phys. Rev. B. 74, 155435-1-8 (2006).
[Crossref]

Gippius, N. A.

A. Christ, T. Zentgraf, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Controlling the interaction between localized and delocalized surface plasmon modes: Experiment and numerical calculations,” Phys. Rev. B. 74, 155435-1-8 (2006).
[Crossref]

Grann, E.B.

Greenwald, A.

I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
[Crossref]

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

Greenwald, A. C.

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Greffet, J. J.

Greffet, J.J.

F. Marquier, K. Joulain, J.P. Mulet, R. Carminati, J.J. Greffet, and Y. Chen, “Coherent spontaneous emission of light by thermal sources,” Phys. Rev. B 69, 155412-1-11 (2004).
[Crossref]

J.J. Greffet, R. Carminati, K. Joulain, J.P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature,  416, 61–64 (2002).
[Crossref] [PubMed]

Grillot, F.

L. Salomon, F. Grillot, A. V. Zayats, and F. de Fornel, “Near-Field Distribution of Optical Transmission of Periodic Subwavelength Holes in a Metal Film,” Phys. Rev. Lett. 86, 1110–1113 (2001).
[Crossref] [PubMed]

Hashizume, J.

J. Hashizume and F. Koyama, “Plasmon Enhanced Optical Near-field Probing of Metal Nanoaperture Surface Emitting Laser,” Opt. Express. 12, 6391–6396 (2004).
[Crossref] [PubMed]

Herminghaus, S.

M. Kreiter, J. Oster, R. Sambles, S. Herminghaus, S. Mittler-Neher, and W. Knoll, “Thermally induced emission of light from a metallic diffraction grating, mediated by surface plasmons,” Opt. Commun. 168, 117–122 (1999)
[Crossref]

Howell, J.

R. Siegel and J. Howell, Thermal Radiation Heat Transfer (New York: Hemisphere Publishing Corporation, 1981).

Ishihara, T.

X. Luo and T. Ishihara, “Surface plasmon resonant interference nanolithography technique,” Appl. Phys. Lett. 84, 4780–4782 (2004)
[Crossref]

Johnson, E.

I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
[Crossref]

Johnson, E. A.

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Joulain, K.

F. Marquier, K. Joulain, J.P. Mulet, R. Carminati, J.J. Greffet, and Y. Chen, “Coherent spontaneous emission of light by thermal sources,” Phys. Rev. B 69, 155412-1-11 (2004).
[Crossref]

J.J. Greffet, R. Carminati, K. Joulain, J.P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature,  416, 61–64 (2002).
[Crossref] [PubMed]

Kassakian, J.

I. Celanovic, D. Perreault, and J. Kassakian, “Resonant-cavity enhanced thermal emission,” Phys. Rev. B 72, 075127-1-6 (2005).
[Crossref]

Knoll, W.

M. Kreiter, J. Oster, R. Sambles, S. Herminghaus, S. Mittler-Neher, and W. Knoll, “Thermally induced emission of light from a metallic diffraction grating, mediated by surface plasmons,” Opt. Commun. 168, 117–122 (1999)
[Crossref]

Koyama, F.

J. Hashizume and F. Koyama, “Plasmon Enhanced Optical Near-field Probing of Metal Nanoaperture Surface Emitting Laser,” Opt. Express. 12, 6391–6396 (2004).
[Crossref] [PubMed]

Kreiter, M.

M. Kreiter, J. Oster, R. Sambles, S. Herminghaus, S. Mittler-Neher, and W. Knoll, “Thermally induced emission of light from a metallic diffraction grating, mediated by surface plasmons,” Opt. Commun. 168, 117–122 (1999)
[Crossref]

Kuhl, J.

A. Christ, T. Zentgraf, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Controlling the interaction between localized and delocalized surface plasmon modes: Experiment and numerical calculations,” Phys. Rev. B. 74, 155435-1-8 (2006).
[Crossref]

Laroche, M.

Lee, S. C.

T. H. Chuang, M. W. Tsai, Y. T. Chang, and S. C. Lee, “Remotely coupled surface plasmons in a two-colored plasmonic thermal emitter,” App. Phys. Lett. 89, 173128–173130 (2006).
[Crossref]

M. W. Tsai, T. H. Chuang, C. Y. Meng, Y. T. Chang, and S. C. Lee, “High performance midinfrared narrow-band plasmonic thermal emitter,” App. Phys. Lett. 89, 173116–173118 (2006).
[Crossref]

Lezec, H. J.

L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001).
[Crossref] [PubMed]

T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through subwavelength hole arrays,” Nature 391, 667–669 (1998)
[Crossref]

Lin, S. Y.

S. Y. Lin, J. G. Fleming, and I. El-Kady, “Experimental observation of photonic-crystal emission near a photonic band edge,” Appl. Phys. Lett. 83, 593–595 (2003).
[Crossref]

S. Y. Lin, J. Moreno, and J. G. Fleming, “A 3D Photonic-Crystal Emitter for Thermal Photovoltaic Generation,” Appl. Phys. Lett. 83, 380–382 (2003).
[Crossref]

Luo, X.

X. Luo and T. Ishihara, “Surface plasmon resonant interference nanolithography technique,” Appl. Phys. Lett. 84, 4780–4782 (2004)
[Crossref]

Mainguy, S.

J.J. Greffet, R. Carminati, K. Joulain, J.P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature,  416, 61–64 (2002).
[Crossref] [PubMed]

Marquier, F.

M. Laroche, C. Arnold, F. Marquier, R. Carminati, J. J. Greffet, S. Collin, N. Bardou, and J. L. Pelouard, “Highly directional radiation generated by a tungsten thermal source,” Opt. Lett. 30, 2623–2625 (2005).
[Crossref] [PubMed]

F. Marquier, K. Joulain, J.P. Mulet, R. Carminati, J.J. Greffet, and Y. Chen, “Coherent spontaneous emission of light by thermal sources,” Phys. Rev. B 69, 155412-1-11 (2004).
[Crossref]

Martin-Moreno, L.

L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001).
[Crossref] [PubMed]

McNeal, M.

I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
[Crossref]

McNeal, M. P.

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Meng, C. Y.

M. W. Tsai, T. H. Chuang, C. Y. Meng, Y. T. Chang, and S. C. Lee, “High performance midinfrared narrow-band plasmonic thermal emitter,” App. Phys. Lett. 89, 173116–173118 (2006).
[Crossref]

Mittler-Neher, S.

M. Kreiter, J. Oster, R. Sambles, S. Herminghaus, S. Mittler-Neher, and W. Knoll, “Thermally induced emission of light from a metallic diffraction grating, mediated by surface plasmons,” Opt. Commun. 168, 117–122 (1999)
[Crossref]

Moelders, N.

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Moharam, M.G.

Moreno, J.

S. Y. Lin, J. Moreno, and J. G. Fleming, “A 3D Photonic-Crystal Emitter for Thermal Photovoltaic Generation,” Appl. Phys. Lett. 83, 380–382 (2003).
[Crossref]

Mukai, T.

K. Okamoto, I. Niki, A. Shvartser, Y. Narukawa, T. Mukai, and A. Scherer, “Surface-plasmon-enhanced light emitters based on InGaN quantum wells,” Nat. Mater. 3, 601–605 (2004).
[Crossref] [PubMed]

Mulet, J.P.

F. Marquier, K. Joulain, J.P. Mulet, R. Carminati, J.J. Greffet, and Y. Chen, “Coherent spontaneous emission of light by thermal sources,” Phys. Rev. B 69, 155412-1-11 (2004).
[Crossref]

J.J. Greffet, R. Carminati, K. Joulain, J.P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature,  416, 61–64 (2002).
[Crossref] [PubMed]

Narukawa, Y.

K. Okamoto, I. Niki, A. Shvartser, Y. Narukawa, T. Mukai, and A. Scherer, “Surface-plasmon-enhanced light emitters based on InGaN quantum wells,” Nat. Mater. 3, 601–605 (2004).
[Crossref] [PubMed]

Ni, B.

P. Ben-Abdallah and B. Ni, “Single-defect Bragg stacks for high-power narrow-band thermal emission,” J. Appl. Phys. 97, 104910-1-5 (2005).
[Crossref]

Nieto-Vesperinas, M.

Niki, I.

K. Okamoto, I. Niki, A. Shvartser, Y. Narukawa, T. Mukai, and A. Scherer, “Surface-plasmon-enhanced light emitters based on InGaN quantum wells,” Nat. Mater. 3, 601–605 (2004).
[Crossref] [PubMed]

Okamoto, K.

K. Okamoto, I. Niki, A. Shvartser, Y. Narukawa, T. Mukai, and A. Scherer, “Surface-plasmon-enhanced light emitters based on InGaN quantum wells,” Nat. Mater. 3, 601–605 (2004).
[Crossref] [PubMed]

Oster, J.

M. Kreiter, J. Oster, R. Sambles, S. Herminghaus, S. Mittler-Neher, and W. Knoll, “Thermally induced emission of light from a metallic diffraction grating, mediated by surface plasmons,” Opt. Commun. 168, 117–122 (1999)
[Crossref]

Palik, E. D.

E. D. Palik, Handbook of Optical Constants of Solids (Academic Press, Boston, 1985).

Pellerin, K. M.

L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001).
[Crossref] [PubMed]

Pelouard, J. L.

Pendry, J. B.

L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001).
[Crossref] [PubMed]

Perreault, D.

I. Celanovic, D. Perreault, and J. Kassakian, “Resonant-cavity enhanced thermal emission,” Phys. Rev. B 72, 075127-1-6 (2005).
[Crossref]

Pommet, D.A.

Pralle, M.

I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
[Crossref]

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

Pralle, M. U.

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Puscasu, I.

I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
[Crossref]

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

Salomon, L.

L. Salomon, F. Grillot, A. V. Zayats, and F. de Fornel, “Near-Field Distribution of Optical Transmission of Periodic Subwavelength Holes in a Metal Film,” Phys. Rev. Lett. 86, 1110–1113 (2001).
[Crossref] [PubMed]

Sambles, R.

M. Kreiter, J. Oster, R. Sambles, S. Herminghaus, S. Mittler-Neher, and W. Knoll, “Thermally induced emission of light from a metallic diffraction grating, mediated by surface plasmons,” Opt. Commun. 168, 117–122 (1999)
[Crossref]

Scherer, A.

K. Okamoto, I. Niki, A. Shvartser, Y. Narukawa, T. Mukai, and A. Scherer, “Surface-plasmon-enhanced light emitters based on InGaN quantum wells,” Nat. Mater. 3, 601–605 (2004).
[Crossref] [PubMed]

Shvartser, A.

K. Okamoto, I. Niki, A. Shvartser, Y. Narukawa, T. Mukai, and A. Scherer, “Surface-plasmon-enhanced light emitters based on InGaN quantum wells,” Nat. Mater. 3, 601–605 (2004).
[Crossref] [PubMed]

Siegel, R.

R. Siegel and J. Howell, Thermal Radiation Heat Transfer (New York: Hemisphere Publishing Corporation, 1981).

Su, M. F.

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

Thio, T.

L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001).
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[Crossref]

Tikhodeev, S. G.

A. Christ, T. Zentgraf, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Controlling the interaction between localized and delocalized surface plasmon modes: Experiment and numerical calculations,” Phys. Rev. B. 74, 155435-1-8 (2006).
[Crossref]

Tsai, M. W.

M. W. Tsai, T. H. Chuang, C. Y. Meng, Y. T. Chang, and S. C. Lee, “High performance midinfrared narrow-band plasmonic thermal emitter,” App. Phys. Lett. 89, 173116–173118 (2006).
[Crossref]

T. H. Chuang, M. W. Tsai, Y. T. Chang, and S. C. Lee, “Remotely coupled surface plasmons in a two-colored plasmonic thermal emitter,” App. Phys. Lett. 89, 173128–173130 (2006).
[Crossref]

Wolff, P. A.

T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through subwavelength hole arrays,” Nature 391, 667–669 (1998)
[Crossref]

Ye, Y.

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

Zayats, A. V.

S. A. Darmanyan and A. V. Zayats, “Light tunneling via resonant surface plasmon polariton states and the enhanced transmission of periodically nanostructured metal films: An analytical study,” Phys. Rev. B 67, 035424-1-7 (2003).
[Crossref]

L. Salomon, F. Grillot, A. V. Zayats, and F. de Fornel, “Near-Field Distribution of Optical Transmission of Periodic Subwavelength Holes in a Metal Film,” Phys. Rev. Lett. 86, 1110–1113 (2001).
[Crossref] [PubMed]

Zentgraf, T.

A. Christ, T. Zentgraf, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Controlling the interaction between localized and delocalized surface plasmon modes: Experiment and numerical calculations,” Phys. Rev. B. 74, 155435-1-8 (2006).
[Crossref]

App. Phys. Lett. (2)

M. W. Tsai, T. H. Chuang, C. Y. Meng, Y. T. Chang, and S. C. Lee, “High performance midinfrared narrow-band plasmonic thermal emitter,” App. Phys. Lett. 89, 173116–173118 (2006).
[Crossref]

T. H. Chuang, M. W. Tsai, Y. T. Chang, and S. C. Lee, “Remotely coupled surface plasmons in a two-colored plasmonic thermal emitter,” App. Phys. Lett. 89, 173128–173130 (2006).
[Crossref]

Appl. Phys. Lett. (4)

M. U. Pralle, N. Moelders, M. P. McNeal, I. Puscasu, A. C. Greenwald, J. T. Daly, E. A. Johnson, T. George, D. S. Choi, I. El-Kady, and R. Biswas, “Photonic crystal enhanced narrow-band infrared emitters,” Appl. Phys. Lett. 81, 4685–4687 (2002).
[Crossref]

S. Y. Lin, J. Moreno, and J. G. Fleming, “A 3D Photonic-Crystal Emitter for Thermal Photovoltaic Generation,” Appl. Phys. Lett. 83, 380–382 (2003).
[Crossref]

S. Y. Lin, J. G. Fleming, and I. El-Kady, “Experimental observation of photonic-crystal emission near a photonic band edge,” Appl. Phys. Lett. 83, 593–595 (2003).
[Crossref]

X. Luo and T. Ishihara, “Surface plasmon resonant interference nanolithography technique,” Appl. Phys. Lett. 84, 4780–4782 (2004)
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J. Appl. Phys. (2)

P. Ben-Abdallah and B. Ni, “Single-defect Bragg stacks for high-power narrow-band thermal emission,” J. Appl. Phys. 97, 104910-1-5 (2005).
[Crossref]

I. Puscasu, M. Pralle, M. McNeal, J. Daly, A. Greenwald, E. Johnson, R. Biswas, and C. G. Ding, “Extraordinary emission from two-dimensional plasmonic-photonic crystals,” J. Appl. Phys. 98, 013531-1-6 (2005).
[Crossref]

J. Mod. Opt. (1)

W. L. Barnes, “Fluorescence near interfaces: the role of photonic mode density,” J. Mod. Opt. 45, 661–699 (1998).
[Crossref]

J. Opt. Soc. Am. A (2)

Nat. Mater. (1)

K. Okamoto, I. Niki, A. Shvartser, Y. Narukawa, T. Mukai, and A. Scherer, “Surface-plasmon-enhanced light emitters based on InGaN quantum wells,” Nat. Mater. 3, 601–605 (2004).
[Crossref] [PubMed]

Nature (2)

T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through subwavelength hole arrays,” Nature 391, 667–669 (1998)
[Crossref]

J.J. Greffet, R. Carminati, K. Joulain, J.P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature,  416, 61–64 (2002).
[Crossref] [PubMed]

Opt. Commun. (1)

M. Kreiter, J. Oster, R. Sambles, S. Herminghaus, S. Mittler-Neher, and W. Knoll, “Thermally induced emission of light from a metallic diffraction grating, mediated by surface plasmons,” Opt. Commun. 168, 117–122 (1999)
[Crossref]

Opt. Express. (1)

J. Hashizume and F. Koyama, “Plasmon Enhanced Optical Near-field Probing of Metal Nanoaperture Surface Emitting Laser,” Opt. Express. 12, 6391–6396 (2004).
[Crossref] [PubMed]

Opt. Lett. (1)

Photonics Nanostruct. Fundam. Appl. (1)

I. El-Kady, R. Biswas, Y. Ye, M. F. Su, I. Puscasu, M. Pralle, E. A. Johnson, J. Daly, and A. Greenwald, Photonics Nanostruct. Fundam. Appl. 1, 69–71 (2003).
[Crossref]

Phys. Rev. B (3)

I. Celanovic, D. Perreault, and J. Kassakian, “Resonant-cavity enhanced thermal emission,” Phys. Rev. B 72, 075127-1-6 (2005).
[Crossref]

S. A. Darmanyan and A. V. Zayats, “Light tunneling via resonant surface plasmon polariton states and the enhanced transmission of periodically nanostructured metal films: An analytical study,” Phys. Rev. B 67, 035424-1-7 (2003).
[Crossref]

F. Marquier, K. Joulain, J.P. Mulet, R. Carminati, J.J. Greffet, and Y. Chen, “Coherent spontaneous emission of light by thermal sources,” Phys. Rev. B 69, 155412-1-11 (2004).
[Crossref]

Phys. Rev. B. (1)

A. Christ, T. Zentgraf, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Controlling the interaction between localized and delocalized surface plasmon modes: Experiment and numerical calculations,” Phys. Rev. B. 74, 155435-1-8 (2006).
[Crossref]

Phys. Rev. Lett. (2)

L. Martin-Moreno, F. J. Garcia-Vidal, H. J. Lezec, K. M. Pellerin, T. Thio, J. B. Pendry, and T. W. Ebbesen, “Theory of Extraordinary Optical Transmission through Subwavelength Hole Arrays,” Phys. Rev. Lett. 86, 1114–1117 (2001).
[Crossref] [PubMed]

L. Salomon, F. Grillot, A. V. Zayats, and F. de Fornel, “Near-Field Distribution of Optical Transmission of Periodic Subwavelength Holes in a Metal Film,” Phys. Rev. Lett. 86, 1110–1113 (2001).
[Crossref] [PubMed]

Other (2)

E. D. Palik, Handbook of Optical Constants of Solids (Academic Press, Boston, 1985).

R. Siegel and J. Howell, Thermal Radiation Heat Transfer (New York: Hemisphere Publishing Corporation, 1981).

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Figures (4)

Fig. 1.
Fig. 1. Basic geometry of an IR emitter considered. It is a plasmonic multilayer structure consisting of a relief metallic grating, a waveguide layer, and a metallic substrate.
Fig. 2.
Fig. 2. Angle-dependent reflectance spectra of the IR emitter. (a) measured. (b) RCWA simulation. The geometric parameters used in the simulation were: Λ=3000nm, =1900nm, tg =100nm and tw =25nm.
Fig. 3.
Fig. 3. Magnetic field strength, Hy 2, (a) along the x-axis at the center of the Ag ridge (b) along the z-axis at the grating/SiO2 interface. The dips at 0.17eV (square) and 0.38eV (triangle) are calculated for an incident angle of 0o while the dips at 0.27eV (circular) and 0.5eV (star) are calculated for an incident angle of 89°. The geometric parameters were: Λ=3000nm, =1900nm, tg =100nm and tw =25nm.
Fig. 4.
Fig. 4. (a) Simulated (dashed line) and measured (solid line) emission spectrum of the IR emitter for 220°C (red line) and 260°C (black line), respectively. The geometric parameters were: Λ=3000nm, =1900nm, tg =100nm and tw =25nm.

Equations (1)

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Emission ( λ ) = TR ( λ ) ( 1 0 π 2 R ( λ , θ ) cos ( θ ) )

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