Abstract

Spectral, spatial, and polarization selective perfect absorption of light in periodic metal-dielectric-metal nanoslits, each of which supporting a single electric-field anti-symmetric surface mode, is systematically studied. Our numerical analysis shows complete absorption of p-polarized light associated with large magnetic field enhancement at wavelengths from the visible to the mid-infrared range and roles played by the geometrical parameters of the structure. This understanding is then applied to the design of the structure with multiple nanoslits in a period that exhibits complete absorption at multiple wavelengths. Semi-analytical expression of the zeroth mode reflectance is derived, which shows a good agreement with numerical simulations and yields clear insight into the underlying physics of light-matter interactions in the structure.

© 2019 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

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2018 (4)

S. J. Kim, J.-H. Kang, M. Mutlu, J. Park, W. Park, K. E. Goodson, R. Sinclair, S. Fan, P. G. Kik, and M. L. Brongersma, “Anti-Hermitian photodetector facilitating efficient subwavelength photon sorting,” Nat. Commun. 9(1), 316 (2018).
[Crossref] [PubMed]

Y. Tsurimaki, J. K. Tong, V. N. Boriskin, A. Semenov, M. I. Ayzatsky, Y. P. Machekhin, G. Chen, and S. V. Boriskina, “Topological Engineering of Interfacial Optical Tamm States for Highly Sensitive Near-Singular-Phase Optical Detection,” ACS Photonics 5(3), 929–938 (2018).
[Crossref]

S. V. Boriskina and Y. Tsurimaki, “Sensitive singular-phase optical detection without phase measurements with Tamm plasmons,” J. Phys. Condens. Matter 30(22), 224003 (2018).
[Crossref] [PubMed]

M. I. Stockman, K. Kneipp, S. I. Bozhevolnyi, S. Saha, A. Dutta, J. Ndukaife, N. Kinsey, H. Reddy, U. Guler, V. M. Shalaev, A. Boltasseva, B. Gholipour, H. N. S. Krishnamoorthy, K. F. MacDonald, C. Soci, N. I. Zheludev, V. Savinov, R. Singh, P. Groß, C. Lienau, M. Vadai, M. L. Solomon, D. R. Barton, M. Lawrence, J. A. Dionne, S. V. Boriskina, R. Esteban, J. Aizpurua, X. Zhang, S. Yang, D. Wang, W. Wang, T. W. Odom, N. Accanto, P. M. de Roque, I. M. Hancu, L. Piatkowski, N. F. van Hulst, and M. F. Kling, “Roadmap on plasmonics,” J. Opt. 20(4), 043001 (2018).
[Crossref]

2017 (2)

S. V. Boriskina, T. A. Cooper, L. Zeng, G. Ni, J. K. Tong, Y. Tsurimaki, Y. Huang, L. Meroueh, G. Mahan, and G. Chen, “Losses in plasmonics: from mitigating energy dissipation to embracing loss-enabled functionalities,” Adv. Opt. Photonics 9(4), 775 (2017).
[Crossref]

M. Zhang, J. Fang, F. Zhang, J. Chen, and H. Yu, “Ultra-narrow band perfect absorbers based on Fano resonance in MIM metamaterials,” Opt. Commun. 405, 216–221 (2017).
[Crossref]

2016 (4)

Z. Yong, S. Zhang, C. Gong, and S. He, “Narrow band perfect absorber for maximum localized magnetic and electric field enhancement and sensing applications,” Sci. Rep. 6(1), 24063 (2016).
[Crossref] [PubMed]

S. V. Boriskina, J. K. Tong, W.-C. Hsu, B. Liao, Y. Huang, V. Chiloyan, and G. Chen, “Heat meets light on the nanoscale,” Nanophotonics 5(1), 134–160 (2016).
[Crossref]

D. M. Bierman, A. Lenert, W. R. Chan, B. Bhatia, I. Celanović, M. Soljačić, and E. N. Wang, “Enhanced photovoltaic energy conversion using thermally based spectral shaping,” Nat. Energy 1(6), 16068 (2016).
[Crossref]

S. V. Boriskina, M. A. Green, K. Catchpole, E. Yablonovitch, M. C. Beard, Y. Okada, S. Lany, T. Gershon, A. Zakutayev, M. H. Tahersima, V. J. Sorger, M. J. Naughton, K. Kempa, M. Dagenais, Y. Yao, L. Xu, X. Sheng, N. D. Bronstein, J. A. Rogers, A. P. Alivisatos, R. G. Nuzzo, J. M. Gordon, D. M. Wu, M. D. Wisser, A. Salleo, J. Dionne, P. Bermel, J.-J. Greffet, I. Celanovic, M. Soljacic, A. Manor, C. Rotschild, A. Raman, L. Zhu, S. Fan, and G. Chen, “Roadmap on optical energy conversion,” J. Opt. 18(7), 073004 (2016).
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2015 (5)

J. K. Tong, W.-C. Hsu, Y. Huang, S. V. Boriskina, and G. Chen, “Thin-film “Thermal Well” emitters and absorbers for high-efficiency thermophotovoltaics,” Sci. Rep. 5(1), 10661 (2015).
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P. Bermel, S. V. Boriskina, Z. Yu, and K. Joulain, “Control of radiative processes for energy conversion and harvesting,” Opt. Express 23(24), A1533–A1540 (2015).
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M. Li, S. K. Cushing, and N. Wu, “Plasmon-enhanced optical sensors: a review,” Analyst (Lond.) 140(2), 386–406 (2015).
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D. Costantini, A. Lefebvre, A.-L. Coutrot, I. Moldovan-Doyen, J.-P. Hugonin, S. Boutami, F. Marquier, H. Benisty, and J.-J. Greffet, “Plasmonic Metasurface for Directional and Frequency-Selective Thermal Emission,” Phys. Rev. Appl. 4(1), 014023 (2015).
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H. U. Yang, J. D’Archangel, M. L. Sundheimer, E. Tucker, G. D. Boreman, and M. B. Raschke, “Optical dielectric function of silver,” Phys. Rev. B Condens. Matter Mater. Phys. 91(23), 235137 (2015).
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2014 (6)

L. Meng, D. Zhao, Z. Ruan, Q. Li, Y. Yang, and M. Qiu, “Optimized grating as an ultra-narrow band absorber or plasmonic sensor,” Opt. Lett. 39(5), 1137–1140 (2014).
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P. C. Wu, G. Sun, W. T. Chen, K.-Y. Yang, Y.-W. Huang, Y.-H. Chen, H. L. Huang, W.-L. Hsu, H. P. Chiang, and D. P. Tsai, “Vertical split-ring resonator based nanoplasmonic sensor,” Appl. Phys. Lett. 105(3), 033105 (2014).
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Z. Li, S. Butun, and K. Aydin, “Ultranarrow Band Absorbers Based on Surface Lattice Resonances in Nanostructured Metal Surfaces,” ACS Nano 8(8), 8242–8248 (2014).
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M. L. Brongersma, Y. Cui, and S. Fan, “Light management for photovoltaics using high-index nanostructures,” Nat. Mater. 13(5), 451–460 (2014).
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M. C. Beard, J. M. Luther, and A. J. Nozik, “The promise and challenge of nanostructured solar cells,” Nat. Nanotechnol. 9(12), 951–954 (2014).
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Y. Nam, Y. X. Yeng, A. Lenert, P. Bermel, I. Celanovic, M. Soljačić, and E. N. Wang, “Solar thermophotovoltaic energy conversion systems with two-dimensional tantalum photonic crystal absorbers and emitters,” Sol. Energy Mater. Sol. Cells 122, 287–296 (2014).
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2013 (3)

S. Molesky, C. J. Dewalt, and Z. Jacob, “High temperature epsilon-near-zero and epsilon-near-pole metamaterial emitters for thermophotovoltaics,” Opt. Express 21(S1), A96–A110 (2013).
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A. Sobhani, M. W. Knight, Y. Wang, B. Zheng, N. S. King, L. V. Brown, Z. Fang, P. Nordlander, and N. J. Halas, “Narrowband photodetection in the near-infrared with a plasmon-induced hot electron device,” Nat. Commun. 4(1), 1643 (2013).
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M. Lorente-Crespo, L. Wang, R. Ortuño, C. García-Meca, Y. Ekinci, and A. Martínez, “Magnetic Hot Spots in Closely Spaced Thick Gold Nanorings,” Nano Lett. 13(6), 2654–2661 (2013).
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2012 (4)

M. G. Nielsen, A. Pors, O. Albrektsen, and S. I. Bozhevolnyi, “Efficient absorption of visible radiation by gap plasmon resonators,” Opt. Express 20(12), 13311–13319 (2012).
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E. Hasman, V. Kleiner, N. Dahan, Y. Gorodetski, K. Frischwasser, and I. Balin, “Manipulation of thermal emission by use of micro and nanoscale structures,” J. Heat Transfer 134(3), 031023 (2012).
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Y. Huang, C. Min, and G. Veronis, “Compact slit-based couplers for metal-dielectric-metal plasmonic waveguides,” Opt. Express 20(20), 22233–22244 (2012).
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C. M. Watts, X. Liu, and W. J. Padilla, “Metamaterial Electromagnetic Wave Absorbers,” Adv. Mater. 24(23), OP181 (2012).
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2011 (4)

C. Min, L. Yang, and G. Veronis, “Microcavity enhanced optical absorption in subwavelength slits,” Opt. Express 19(27), 26850–26858 (2011).
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K. Aydin, V. E. Ferry, R. M. Briggs, and H. A. Atwater, “Broadband polarization-independent resonant light absorption using ultrathin plasmonic super absorbers,” Nat. Commun. 2(1), 517 (2011).
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M. G. Nielsen, D. K. Gramotnev, A. Pors, O. Albrektsen, and S. I. Bozhevolnyi, “Continuous layer gap plasmon resonators,” Opt. Express 19(20), 19310–19322 (2011).
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J. Hao, L. Zhou, and M. Qiu, “Nearly total absorption of light and heat generation by plasmonic metamaterials,” Phys. Rev. B Condens. Matter Mater. Phys. 83(16), 165107 (2011).
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2010 (6)

2009 (4)

I. S. Spevak, A. Y. Nikitin, E. V. Bezuglyi, A. Levchenko, and A. V. Kats, “Resonantly suppressed transmission and anomalously enhanced light absorption in periodically modulated ultrathin metal films,” Phys. Rev. B Condens. Matter Mater. Phys. 79(16), 161406 (2009).
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P. Berini, “Long-range surface plasmon polaritons,” Adv. Opt. Photonics 1(3), 484 (2009).
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J. S. White, G. Veronis, Z. Yu, E. S. Barnard, A. Chandran, S. Fan, and M. L. Brongersma, “Extraordinary optical absorption through subwavelength slits,” Opt. Lett. 34(5), 686–688 (2009).
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A. Gopinath, S. V. Boriskina, B. M. Reinhard, and L. Dal Negro, “Deterministic aperiodic arrays of metal nanoparticles for surface-enhanced Raman scattering (SERS),” Opt. Express 17(5), 3741–3753 (2009).
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2008 (5)

J. Le Perchec, P. Quémerais, A. Barbara, and T. López-Ríos, “Why Metallic Surfaces with Grooves a Few Nanometers Deep and Wide May Strongly Absorb Visible Light,” Phys. Rev. Lett. 100(6), 066408 (2008).
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V. G. Kravets, F. Schedin, and A. N. Grigorenko, “Plasmonic blackbody: Almost complete absorption of light in nanostructured metallic coatings,” Phys. Rev. B Condens. Matter Mater. Phys. 78(20), 205405 (2008).
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E. Popov, D. Maystre, R. C. McPhedran, M. Nevière, M. C. Hutley, and G. H. Derrick, “Total absorption of unpolarized light by crossed gratings,” Opt. Express 16(9), 6146–6155 (2008).
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N. I. Landy, S. Sajuyigbe, J. J. Mock, D. R. Smith, and W. J. Padilla, “Perfect Metamaterial Absorber,” Phys. Rev. Lett. 100(20), 207402 (2008).
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L. Tsakalakos, “Nanostructures for photovoltaics,” Mater. Sci. Eng. Rep. 62(6), 175–189 (2008).
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2007 (1)

S. Lal, S. Link, and N. J. Halas, “Nano-optics from sensing to waveguiding,” Nat. Photonics 1(11), 641–648 (2007).
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2006 (5)

M.-W. Tsai, T.-H. Chuang, C.-Y. Meng, Y.-T. Chang, and S.-C. Lee, “High performance midinfrared narrow-band plasmonic thermal emitter,” Appl. Phys. Lett. 89(17), 173116 (2006).
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A. K. Sarychev, G. Shvets, and V. M. Shalaev, “Magnetic plasmon resonance,” Phys. Rev. E Stat. Nonlin. Soft Matter Phys. 73(3), 036609 (2006).
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H. T. Miyazaki and Y. Kurokawa, “Squeezing Visible Light Waves into a 3-nm-Thick and 55-nm-Long Plasmon Cavity,” Phys. Rev. Lett. 96(9), 097401 (2006).
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J. A. Dionne, L. A. Sweatlock, H. A. Atwater, and A. Polman, “Plasmon slot waveguides: Towards chip-scale propagation with subwavelength-scale localization,” Phys. Rev. B Condens. Matter Mater. Phys. 73(3), 035407 (2006).
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R. Gordon, “Light in a subwavelength slit in a metal: Propagation and reflection,” Phys. Rev. B Condens. Matter Mater. Phys. 73(15), 153405 (2006).
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2005 (4)

D.-K. Qing and G. Chen, “Nanoscale optical waveguides with negative dielectric claddings,” Phys. Rev. B Condens. Matter Mater. Phys. 71(15), 153107 (2005).
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H. Sai, Y. Kanamori, and H. Yugami, “Tuning of the thermal radiation spectrum in the near-infrared region by metallic surface microstructures,” J. Micromech. Microeng. 15(9), S243–S249 (2005).
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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(19), 2623–2625 (2005).
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T. V. Teperik, V. V. Popov, and F. J. García de Abajo, “Void plasmons and total absorption of light in nanoporous metallic films,” Phys. Rev. B Condens. Matter Mater. Phys. 71(8), 085408 (2005).
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2004 (1)

F. Marquier, K. Joulain, J. P. Mulet, R. Carminati, and J. J. Greffet, “Engineering infrared emission properties of silicon in the near field and the far field,” Opt. Commun. 237(4–6), 379–388 (2004).
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2003 (2)

W. L. Barnes, A. Dereux, and T. W. Ebbesen, “Surface plasmon subwavelength optics,” Nature 424(6950), 824–830 (2003).
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F. J. García-Vidal, H. J. Lezec, T. W. Ebbesen, and L. Martín-Moreno, “Multiple Paths to Enhance Optical Transmission through a Single Subwavelength Slit,” Phys. Rev. Lett. 90(21), 213901 (2003).
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2002 (3)

K. Kneipp, H. Kneipp, I. Itzkan, R. R. Dasari, and M. S. Feld, “Surface-enhanced Raman scattering and biophysics,” J. Phys. Condens. Matter 14(18), 202 (2002).
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J.-J. Greffet, R. Carminati, K. Joulain, J.-P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature 416(6876), 61–64 (2002).
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J.-J. Greffet, R. Carminati, K. Joulain, J.-P. Mulet, S. Mainguy, and Y. Chen, “Coherent emission of light by thermal sources,” Nature 416(6876), 61–64 (2002).
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2001 (1)

L. Martín-Moreno, F. J. García-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(6), 1114–1117 (2001).
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2000 (1)

P. Lalanne, J. P. Hugonin, S. Astilean, M. Palamaru, and K. D. Möller, “One-mode model and Airy-like formulae for one-dimensional metallic gratings,” J. Opt. A, Pure Appl. Opt. 2(1), 48–51 (2000).
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1999 (2)

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(1–4), 117–122 (1999).
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T. J. Coutts, “A review of progress in thermophotovoltaic generation of electricity,” Renew. Sustain. Energy Rev. 3(2–3), 77–184 (1999).
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1998 (1)

T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through sub-wavelength hole arrays,” Nature 391(6668), 667–669 (1998).
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1997 (1)

K. Kneipp, Y. Wang, H. Kneipp, L. T. Perelman, I. Itzkan, R. R. Dasari, and M. S. Feld, “Single Molecule Detection Using Surface-Enhanced Raman Scattering (SERS),” Phys. Rev. Lett. 78(9), 1667–1670 (1997).
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1992 (1)

E. Betzig and J. K. Trautman, "Near-field optics: microscopy, spectroscopy, and surface modification beyond the diffraction limit," Science 257(5067), 189-195 (1992)

1991 (1)

B. Prade, J. Y. Vinet, and A. Mysyrowicz, “Guided optical waves in planar heterostructures with negative dielectric constant,” Phys. Rev. B Condens. Matter 44(24), 13556–13572 (1991).
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1981 (3)

L. C. Botten, M. S. Craig, and R. C. McPhedran, “Highly Conducting Lamellar Diffraction Gratings,” Opt. Acta (Lond.) 28(8), 1103–1106 (1981).
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L. C. Botten, M. S. Craig, R. C. McPhedran, J. L. Adams, and J. R. Andrewartha, “The Finitely Conducting Lamellar Diffraction Grating,” Opt. Acta (Lond.) 28(8), 1087–1102 (1981).
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I. C. Botten, M. S. Craig, R. C. McPhedran, J. L. Adams, and J. R. Andrewartha, “The Dielectric Lamellar Diffraction Grating,” Opt. Acta (Lond.) 28(3), 413–428 (1981).
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1976 (1)

M. C. Hutley and D. Maystre, “The total absorption of light by a diffraction grating,” Opt. Commun. 19(3), 431–436 (1976).
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1965 (2)

A. Hessel and A. A. Oliner, “A New Theory of Wood’s Anomalies on Optical Gratings,” Appl. Opt. 4(10), 1275 (1965).
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J. A. Nelder and R. Mead, “A Simplex Method for Function Minimization,” Comput. J. 7(4), 308–313 (1965).
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1935 (1)

R. W. Wood, “Anomalous Diffraction Gratings,” Phys. Rev. 48(12), 928–936 (1935).
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M. I. Stockman, K. Kneipp, S. I. Bozhevolnyi, S. Saha, A. Dutta, J. Ndukaife, N. Kinsey, H. Reddy, U. Guler, V. M. Shalaev, A. Boltasseva, B. Gholipour, H. N. S. Krishnamoorthy, K. F. MacDonald, C. Soci, N. I. Zheludev, V. Savinov, R. Singh, P. Groß, C. Lienau, M. Vadai, M. L. Solomon, D. R. Barton, M. Lawrence, J. A. Dionne, S. V. Boriskina, R. Esteban, J. Aizpurua, X. Zhang, S. Yang, D. Wang, W. Wang, T. W. Odom, N. Accanto, P. M. de Roque, I. M. Hancu, L. Piatkowski, N. F. van Hulst, and M. F. Kling, “Roadmap on plasmonics,” J. Opt. 20(4), 043001 (2018).
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Adams, J. L.

L. C. Botten, M. S. Craig, R. C. McPhedran, J. L. Adams, and J. R. Andrewartha, “The Finitely Conducting Lamellar Diffraction Grating,” Opt. Acta (Lond.) 28(8), 1087–1102 (1981).
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I. C. Botten, M. S. Craig, R. C. McPhedran, J. L. Adams, and J. R. Andrewartha, “The Dielectric Lamellar Diffraction Grating,” Opt. Acta (Lond.) 28(3), 413–428 (1981).
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Aizpurua, J.

M. I. Stockman, K. Kneipp, S. I. Bozhevolnyi, S. Saha, A. Dutta, J. Ndukaife, N. Kinsey, H. Reddy, U. Guler, V. M. Shalaev, A. Boltasseva, B. Gholipour, H. N. S. Krishnamoorthy, K. F. MacDonald, C. Soci, N. I. Zheludev, V. Savinov, R. Singh, P. Groß, C. Lienau, M. Vadai, M. L. Solomon, D. R. Barton, M. Lawrence, J. A. Dionne, S. V. Boriskina, R. Esteban, J. Aizpurua, X. Zhang, S. Yang, D. Wang, W. Wang, T. W. Odom, N. Accanto, P. M. de Roque, I. M. Hancu, L. Piatkowski, N. F. van Hulst, and M. F. Kling, “Roadmap on plasmonics,” J. Opt. 20(4), 043001 (2018).
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Alivisatos, A. P.

S. V. Boriskina, M. A. Green, K. Catchpole, E. Yablonovitch, M. C. Beard, Y. Okada, S. Lany, T. Gershon, A. Zakutayev, M. H. Tahersima, V. J. Sorger, M. J. Naughton, K. Kempa, M. Dagenais, Y. Yao, L. Xu, X. Sheng, N. D. Bronstein, J. A. Rogers, A. P. Alivisatos, R. G. Nuzzo, J. M. Gordon, D. M. Wu, M. D. Wisser, A. Salleo, J. Dionne, P. Bermel, J.-J. Greffet, I. Celanovic, M. Soljacic, A. Manor, C. Rotschild, A. Raman, L. Zhu, S. Fan, and G. Chen, “Roadmap on optical energy conversion,” J. Opt. 18(7), 073004 (2016).
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I. C. Botten, M. S. Craig, R. C. McPhedran, J. L. Adams, and J. R. Andrewartha, “The Dielectric Lamellar Diffraction Grating,” Opt. Acta (Lond.) 28(3), 413–428 (1981).
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L. C. Botten, M. S. Craig, R. C. McPhedran, J. L. Adams, and J. R. Andrewartha, “The Finitely Conducting Lamellar Diffraction Grating,” Opt. Acta (Lond.) 28(8), 1087–1102 (1981).
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Arnold, C.

Astilean, S.

P. Lalanne, J. P. Hugonin, S. Astilean, M. Palamaru, and K. D. Möller, “One-mode model and Airy-like formulae for one-dimensional metallic gratings,” J. Opt. A, Pure Appl. Opt. 2(1), 48–51 (2000).
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K. Aydin, V. E. Ferry, R. M. Briggs, and H. A. Atwater, “Broadband polarization-independent resonant light absorption using ultrathin plasmonic super absorbers,” Nat. Commun. 2(1), 517 (2011).
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H. A. Atwater and A. Polman, “Plasmonics for improved photovoltaic devices,” Nat. Mater. 9(3), 205–213 (2010).
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J. A. Dionne, L. A. Sweatlock, H. A. Atwater, and A. Polman, “Plasmon slot waveguides: Towards chip-scale propagation with subwavelength-scale localization,” Phys. Rev. B Condens. Matter Mater. Phys. 73(3), 035407 (2006).
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Z. Li, S. Butun, and K. Aydin, “Ultranarrow Band Absorbers Based on Surface Lattice Resonances in Nanostructured Metal Surfaces,” ACS Nano 8(8), 8242–8248 (2014).
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K. Aydin, V. E. Ferry, R. M. Briggs, and H. A. Atwater, “Broadband polarization-independent resonant light absorption using ultrathin plasmonic super absorbers,” Nat. Commun. 2(1), 517 (2011).
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Y. Tsurimaki, J. K. Tong, V. N. Boriskin, A. Semenov, M. I. Ayzatsky, Y. P. Machekhin, G. Chen, and S. V. Boriskina, “Topological Engineering of Interfacial Optical Tamm States for Highly Sensitive Near-Singular-Phase Optical Detection,” ACS Photonics 5(3), 929–938 (2018).
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E. Hasman, V. Kleiner, N. Dahan, Y. Gorodetski, K. Frischwasser, and I. Balin, “Manipulation of thermal emission by use of micro and nanoscale structures,” J. Heat Transfer 134(3), 031023 (2012).
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J. Le Perchec, P. Quémerais, A. Barbara, and T. López-Ríos, “Why Metallic Surfaces with Grooves a Few Nanometers Deep and Wide May Strongly Absorb Visible Light,” Phys. Rev. Lett. 100(6), 066408 (2008).
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J. A. Schuller, E. S. Barnard, W. Cai, Y. C. Jun, J. S. White, and M. L. Brongersma, “Plasmonics for extreme light concentration and manipulation,” Nat. Mater. 9(3), 193–204 (2010).
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W. L. Barnes, A. Dereux, and T. W. Ebbesen, “Surface plasmon subwavelength optics,” Nature 424(6950), 824–830 (2003).
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S. V. Boriskina, M. A. Green, K. Catchpole, E. Yablonovitch, M. C. Beard, Y. Okada, S. Lany, T. Gershon, A. Zakutayev, M. H. Tahersima, V. J. Sorger, M. J. Naughton, K. Kempa, M. Dagenais, Y. Yao, L. Xu, X. Sheng, N. D. Bronstein, J. A. Rogers, A. P. Alivisatos, R. G. Nuzzo, J. M. Gordon, D. M. Wu, M. D. Wisser, A. Salleo, J. Dionne, P. Bermel, J.-J. Greffet, I. Celanovic, M. Soljacic, A. Manor, C. Rotschild, A. Raman, L. Zhu, S. Fan, and G. Chen, “Roadmap on optical energy conversion,” J. Opt. 18(7), 073004 (2016).
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S. V. Boriskina, M. A. Green, K. Catchpole, E. Yablonovitch, M. C. Beard, Y. Okada, S. Lany, T. Gershon, A. Zakutayev, M. H. Tahersima, V. J. Sorger, M. J. Naughton, K. Kempa, M. Dagenais, Y. Yao, L. Xu, X. Sheng, N. D. Bronstein, J. A. Rogers, A. P. Alivisatos, R. G. Nuzzo, J. M. Gordon, D. M. Wu, M. D. Wisser, A. Salleo, J. Dionne, P. Bermel, J.-J. Greffet, I. Celanovic, M. Soljacic, A. Manor, C. Rotschild, A. Raman, L. Zhu, S. Fan, and G. Chen, “Roadmap on optical energy conversion,” J. Opt. 18(7), 073004 (2016).
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P. Bermel, S. V. Boriskina, Z. Yu, and K. Joulain, “Control of radiative processes for energy conversion and harvesting,” Opt. Express 23(24), A1533–A1540 (2015).
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Y. Nam, Y. X. Yeng, A. Lenert, P. Bermel, I. Celanovic, M. Soljačić, and E. N. Wang, “Solar thermophotovoltaic energy conversion systems with two-dimensional tantalum photonic crystal absorbers and emitters,” Sol. Energy Mater. Sol. Cells 122, 287–296 (2014).
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Figures (8)

Fig. 1
Fig. 1 Schematic of periodic nanoslit structure (on the right) and its cross-sectional view on the x-y plane (on the left). Nanoslits formed by a metallic material with dielectric function εm are filled with a dielectric with εd. The substrate is a material with dielectric function εIII and is in general different from the materials in the region II. The incident light is assumed to be on the x-y plane, i.e., the azimuthal angle is zero. Complete absorption is due to coupling to the electric-field anti-symmetric surface mode supported in nanoslits (typical field distribution of the y-component of the electric field is depicted), but not due to propagating SPPs at the surface.
Fig. 2
Fig. 2 (a): Schematic of oscillating modes and surface modes propagating in the y-direction in an infinitely-long MDM waveguide. In oscillating modes, wave propagation is analogous to a mode guided by total internal reflection in a dielectric slab waveguide. For surface modes, typical y-component field distributions of the electric field for symmetric and anti-symmetric surface modes are shown. Dispersion relations of (b) lower and upper cutoff wavelengths of TM0 and TM1 modes, and (c) the anti-symmetric surface polariton mode in the nanoslits and the surface polariton mode supported by a single Si-Ag planar interface.
Fig. 3
Fig. 3 Spectral reflectance of the periodic nanoslit structure for p-polarized normally incident light (θ = 0). The dielectric and the metal in the region II and the substrate are silicon, silver, and silver, respectively. The geometrical parameters of the three structures are also shown. For the dielectric constants of silicon, we use: εSi = 12.75 + i0.002, εSi = 11.79, and εSi = 11.66 + i0.0004 for (a), (b), and (c), respectively, and frequency dispersion of silicon is not considered.
Fig. 4
Fig. 4 Effects of period d and waveguide width w on the spectral reflectance for p-polarized normally incident light. The geometrical parameters are varied from the structure in Fig. 3 (b): d = 1400nm, h = 140nm, and w = 95nm.
Fig. 5
Fig. 5 Comparison of spectral reflectance between the numerical simulation (dots) and the semi-analytical results (solid lines) obtained by Eq. (11) for: (a) structure shown in Fig. 2 (b) and (b) structure shown in Fig. 2 (c). For (a), the propagation constant β is calculated by two methods: the solution of Eq. (2). (red line) and the rigorous mode expansion in FDTD simulation (green line) and for (b), the solution of Eq. (2) is used.
Fig. 6
Fig. 6 Applications of periodic nanoslit structures (a) Electric and magnetic field enhancement (heat maps) at the resonant wavelength of the structure in Fig. 3 (b). The distribution of the Poynting vector is shown as white arrows in the magnetic field plot on the left. The electric current density vector is shown as white arrows in the electric field plot on the right. The vectors are normalized and thus the length of the vectors indicates only the direction, but not the magnitude. (b) Polarization selectivity of spectral reflectance for normal incident light; (c) Angular spectrum of the absorptance (emittance) of the three structures in Fig. 3 at the corresponding resonant frequencies.
Fig. 7
Fig. 7 Complete absorption of light at two different wavelengths supported by two nanoslits. (a) A schematic of the two-nanoslit structure. (b) The spatial distribution of magnetic field normalized by the incident magnetic field at the two resonant wavelengths. (c) The corresponding dual-band reflectance spectrum. For the dielectric constant of silicon, we used εSi = 11.79.
Fig. 8
Fig. 8 Spectral reflectance of periodic nanoslit structure for normally incident p-polarized light with realistic fillets at the edges of the nanoslit. The geometrical parameter, as well as materials, are the same as those in the structure in Fig. 3 (b). The radius of the fillets is w/3.

Equations (12)

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k x d w=2arctan( k x m k x d )+lπ TE l mode k x d w=2arctan( ε m k x d ε d k x m )+lπ TM l mode
1+ ε m k x d ε d k x m tanh( i k x d w 2 )=0
H z I (x,y)= e i( k 0,x I x k 0,y I (yh/2)) + p= r p u p I (x) e i k p,y I (yh/2) yh/2
H z II (x,y)=(asin(βy)+bcos(βy)) u II (x) h/2yh/2
H z III (x,y)= p= t p u p III (x) e i k p,y III (y+h/2) yh/2
k (x) 2 x ( 1 k (x) 2 x u II (x) )+( ε m ε d ) k 0 2 Θ(xw) u II (x)= β 2 u II (x)
k(x)={ ε d k 0 0xw ε m k 0 w<xd Θ(xw)={ 0 x<w 1 x>w
u II (x)=θ(x)+γψ(x)
θ(x)={ cos( k x d x) 0xw cos( k x d w)sin( k x m (xw)) k x d k x m sin( k x d w)sin( k x m (xw)) wxd
ψ(x)={ 1 k x d sin( k x d x) 0xw 1 k x d sin( k x d w)cos( k x m (xw))+ 1 k x m cos( k x d w)sin( k x m (xw)) wxd
r 0 =12i ( β/ k 0,y I ) | A 0 | 2 (coth(βh)+iK) 1MK+i(M+K)coth(βh)
A p = 0 d dx 1 ( k II 2 (x)) ( u p I (x)) u p II (x) k II (x)={ ε d k 0 0xw ε m k 0 wxd

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