Mimicking electromagnetically induced transparency in the magneto-optical activity of magnetoplasmonic nanoresonators

G. Armelles; A. Cebollada; A. García-Martín; M. U. González; F. García; D. Meneses-Rodríguez; N. de Sousa; L. S. Froufe-Pérez

doi:10.1364/OE.21.027356

Mimicking electromagnetically induced transparency in the magneto-optical activity of magnetoplasmonic nanoresonators

G. Armelles, A. Cebollada, A. García-Martín, M. U. González, F. García, D. Meneses-Rodríguez, N. de Sousa, and L. S. Froufe-Pérez

Optics Express
Vol. 21,
Issue 22,
pp. 27356-27370
(2013)
•https://doi.org/10.1364/OE.21.027356

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G. Armelles, A. Cebollada, A. García-Martín, M. U. González, F. García, D. Meneses-Rodríguez, N. de Sousa, and L. S. Froufe-Pérez, "Mimicking electromagnetically induced transparency in the magneto-optical activity of magnetoplasmonic nanoresonators," Opt. Express 21, 27356-27370 (2013)

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Related Topics
Table of Contents Category
- Plasmonics
Optics & Photonics Topics
?

The topics in this list come from the OSA Optics and Photonics Topics applied to this article.
Previously assigned OCIS codes
- Magneto-optical materials (160.3820)
- Magneto-optic systems (230.3810)
- Surface plasmons (240.6680)
- Plasmonics (250.5403)
- Nanophotonics and photonic crystals (350.4238)
- Metal optics (260.3910)

About this Article
History
- Original Manuscript: July 30, 2013
- Revised Manuscript: September 23, 2013
- Manuscript Accepted: September 24, 2013
- Published: November 4, 2013
Virtual Issues
Optics Express Surface Plasmon Photonics (2013)

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Abstract

We show that the interaction between a plasmonic and a magnetoplasmonic metallic nanodisk leads to the appearance of magneto-optical activity in the purely plasmonic disk induced by the magnetoplasmonic one. Moreover, at specific wavelengths the interaction cancels the net electromagnetic field at the magnetoplasmonic component, strongly reducing the magneto-optical activity of the whole system. The MO activity has a characteristic Fano spectral shape, and the resulting MO inhibition constitutes the magneto-optical counterpart of the electromagnetic induced transparency.

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G. Armelles, A. Cebollada, A. García-Martín, and M. U. González, “Magnetoplasmonics: combining magnetic and plasmonic functionalities,” Adv. Opt. Mater. 1(1), 10–35 (2013).
[Crossref]

J. Y. Chin, T. Steinle, T. Wehlus, D. Dregely, T. Weiss, V. I. Belotelov, B. Stritzker, and H. Giessen, “Nonreciprocal plasmonics enables giant enhancement of thin-film Faraday rotation,” Nat Commun 4, 1599 (2013).
[Crossref] [PubMed]

2012 (6)

A. E. Cetin and H. Altug, “Fano resonant ring/disk plasmonic nanocavities on conducting substrates for advanced biosensing,” ACS Nano 6(11), 9989–9995 (2012).
[Crossref] [PubMed]

J. C. Banthí, D. Meneses-Rodríguez, F. García, M. U. González, A. García-Martín, A. Cebollada, and G. Armelles, “High magneto-optical activity and low optical losses in metal-dielectric Au/Co/Au-SiO2 magnetoplasmonic nanodisks,” Adv. Mater. 24(10), OP36–OP41 (2012).
[Crossref] [PubMed]

C. Wadell, T. J. Antosiewicz, and C. Langhammer, “Optical absorption engineering in stacked plasmonic Au-SiO₂-Pd nanoantennas,” Nano Lett. 12(9), 4784–4790 (2012).
[Crossref] [PubMed]

Y. Francescato, V. Giannini, and S. A. Maier, “Plasmonic systems unveiled by Fano resonances,” ACS Nano 6(2), 1830–1838 (2012).
[Crossref] [PubMed]

B. Caballero, A. García-Martín, and J. C. Cuevas, “Generalized scattering-matrix approach for magneto-optics in periodically patterned multilayer systems,” Phys. Rev. B 85(24), 245103 (2012).
[Crossref]

T. J. Antosiewicz, S. P. Apell, C. Wadell, and C. Langhammer, “Absorption enhancement in lossy transition metal elements of plasmonic nanosandwiches,” J. Phys. Chem. C 116(38), 20522–20529 (2012).
[Crossref]

2011 (7)

A. A. Yanik, A. E. Cetin, M. Huang, A. Artar, S. H. Mousavi, A. Khanikaev, J. H. Connor, G. Shvets, and H. Altug, “Seeing protein monolayers with naked eye through plasmonic Fano resonances,” Proc. Natl. Acad. Sci. U.S.A. 108(29), 11784–11789 (2011).
[Crossref] [PubMed]

C. Wu, A. B. Khanikaev, R. Adato, N. Arju, A. A. Yanik, H. Altug, and G. Shvets, “Fano-resonant asymmetric metamaterials for ultrasensitive spectroscopy and identification of molecular monolayers,” Nat. Mater. 11(1), 69–75 (2011).
[Crossref] [PubMed]

P. Offermans, M. C. Schaafsma, S. R. K. Rodriguez, Y. Zhang, M. Crego-Calama, S. H. Brongersma, and J. Gómez Rivas, “Universal scaling of the figure of merit of plasmonic sensors,” ACS Nano 5(6), 5151–5157 (2011).
[Crossref] [PubMed]

V. Bonanni, S. Bonetti, T. Pakizeh, Z. Pirzadeh, J. Chen, J. Nogués, P. Vavassori, R. Hillenbrand, J. Åkerman, and A. Dmitriev, “Designer magnetoplasmonics with nickel nanoferromagnets,” Nano Lett. 11(12), 5333–5338 (2011).
[Crossref] [PubMed]

Z.-J. Yang, Z.-S. Zhang, L.-H. Zhang, Q.-Q. Li, Z.-H. Hao, and Q.-Q. Wang, “Fano resonances in dipole-quadrupole plasmon coupling nanorod dimers,” Opt. Lett. 36(9), 1542–1544 (2011).
[Crossref] [PubMed]

B. Gallinet and O. J. F. Martin, “Influence of electromagnetic interactions on the line shape of plasmonic Fano resonances,” ACS Nano 5(11), 8999–9008 (2011).
[Crossref] [PubMed]

V. I. Belotelov, I. A. Akimov, M. Pohl, V. A. Kotov, S. Kasture, A. S. Vengurlekar, A. V. Gopal, D. R. Yakovlev, A. K. Zvezdin, and M. Bayer, “Enhanced magneto-optical effects in magnetoplasmonic crystals,” Nat. Nanotechnol. 6(6), 370–376 (2011).
[Crossref] [PubMed]

2010 (8)

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).
[Crossref] [PubMed]

V. V. Temnov, G. Armelles, U. Woggon, D. Guzatov, A. Cebollada, A. Garcia-Martin, J. M. Garcia-Martin, T. Thomay, A. Leitenstorfer, and R. Bratschitsch, “Active magneto-plasmonics in hybrid metal-ferromagnet structures,” Nat. Photonics 4(2), 107–111 (2010).
[Crossref]

B. Sepúlveda, J. B. González-Díaz, A. García-Martín, L. M. Lechuga, and G. Armelles, “Plasmon-induced magneto-optical activity in nanosized gold disks,” Phys. Rev. Lett. 104(14), 147401 (2010).
[Crossref] [PubMed]

L. V. Brown, H. Sobhani, J. B. Lassiter, P. Nordlander, and N. J. Halas, “Heterodimers: plasmonic properties of mismatched nanoparticle pairs,” ACS Nano 4(2), 819–832 (2010).
[Crossref] [PubMed]

B. Luk’yanchuk, N. I. Zheludev, S. A. Maier, N. J. Halas, P. Nordlander, H. Giessen, and C. T. Chong, “The Fano resonance in plasmonic nanostructures and metamaterials,” Nat. Mater. 9(9), 707–715 (2010).
[Crossref] [PubMed]

M. Hentschel, M. Saliba, R. Vogelgesang, H. Giessen, A. P. Alivisatos, and N. Liu, “Transition from isolated to collective modes in plasmonic oligomers,” Nano Lett. 10(7), 2721–2726 (2010).
[Crossref] [PubMed]

J. B. Lassiter, H. Sobhani, J. A. Fan, J. Kundu, F. Capasso, P. Nordlander, and N. J. Halas, “Fano resonances in plasmonic nanoclusters: geometrical and chemical tunability,” Nano Lett. 10(8), 3184–3189 (2010).
[Crossref] [PubMed]

S. Albaladejo, R. Gómez-Medina, L. S. Froufe-Pérez, H. Marinchio, R. Carminati, J. F. Torrado, G. Armelles, A. García-Martín, and J. J. Sáenz, “Radiative corrections to the polarizability tensor of an electrically small anisotropic dielectric particle,” Opt. Express 18(4), 3556–3567 (2010), http://www.opticsexpress.org/abstract.cfm?URI=oe-18-4-3556 .
[Crossref] [PubMed]

2009 (2)

N. Verellen, Y. Sonnefraud, H. Sobhani, F. Hao, V. V. Moshchalkov, P. Van Dorpe, P. Nordlander, and S. A. Maier, “Fano resonances in individual coherent plasmonic nanocavities,” Nano Lett. 9(4), 1663–1667 (2009).
[Crossref] [PubMed]

N. Liu, L. Langguth, T. Weiss, J. Kästel, M. Fleischhauer, T. Pfau, and H. Giessen, “Plasmonic analogue of electromagnetically induced transparency at the Drude damping limit,” Nat. Mater. 8(9), 758–762 (2009).
[Crossref] [PubMed]

2008 (9)

J. B. González-Díaz, A. García-Martín, J. M. García-Martín, A. Cebollada, G. Armelles, B. Sepúlveda, Y. Alaverdyan, and M. Käll, “Plasmonic Au/Co/Au nanosandwiches with enhanced magneto-optical activity,” Small 4(2), 202–205 (2008).
[Crossref] [PubMed]

S. Zhang, D. A. Genov, Y. Wang, M. Liu, and X. Zhang, “Plasmon-induced transparency in metamaterials,” Phys. Rev. Lett. 101(4), 047401 (2008).
[Crossref] [PubMed]

N. Papasimakis, V. A. Fedotov, N. I. Zheludev, and S. L. Prosvirnin, “Metamaterial analog of electromagnetically induced transparency,” Phys. Rev. Lett. 101(25), 253903 (2008).
[Crossref] [PubMed]

E. Cubukcu, Yu. Nanfang, E. J. Smythe, L. Diehl, K. B. Crozier, and F. Capasso, “Plasmonic laser antennas and related devices,” IEEE J. Sel. Top. Quantum Electron. 14(6), 1448–1461 (2008).
[Crossref]

J. N. Anker, W. P. Hall, O. Lyandres, N. C. Shah, J. Zhao, and R. P. Van Duyne, “Biosensing with plasmonic nanosensors,” Nat. Mater. 7(6), 442–453 (2008).
[Crossref] [PubMed]

P. Ghenuche, S. Cherukulappurath, T. H. Taminiau, N. F. van Hulst, and R. Quidant, “Spectroscopic mode mapping of resonant plasmon nanoantennas,” Phys. Rev. Lett. 101(11), 116805 (2008).
[Crossref] [PubMed]

B. Auguié and W. L. Barnes, “Collective resonances in gold nanoparticle arrays,” Phys. Rev. Lett. 101(14), 143902 (2008).
[Crossref] [PubMed]

T. Pakizeh, A. Dmitriev, M. S. Abrishamian, N. Granpayeh, and M. Käll, “Structural asymmetry and induced optical magnetism in plasmonic nanosandwiches,” J. Opt. Soc. Am. B 25(4), 659–667 (2008).
[Crossref]

Y. Ekinci, A. Christ, M. Agio, O. J. F. Martin, H. H. Solak, and J. F. Löffler, “Electric and magnetic resonances in arrays of coupled gold nanoparticle in-tandem pairs,” Opt. Express 16(17), 13287–13295 (2008), http://www.opticsexpress.org/abstract.cfm?URI=oe-16-17-13287 .
[Crossref] [PubMed]

2007 (2)

A. Dmitriev, T. Pakizeh, M. Käll, and D. S. Sutherland, “Gold-silica-gold nanosandwiches: tunable bimodal plasmonic resonators,” Small 3(2), 294–299 (2007).
[Crossref] [PubMed]

H. Fredriksson, Y. Alaverdyan, A. Dmitriev, C. Langhammer, D. S. Sutherland, M. Zäch, and B. Kasemo, “Hole–mask colloidal lithography,” Adv. Mater. 19(23), 4297–4302 (2007).
[Crossref]

2006 (3)

Q. Xu, S. Sandhu, M. L. Povinelli, J. Shakya, S. Fan, and M. Lipson, “Experimental realization of an on-chip all-optical analogue to electromagnetically induced transparency,” Phys. Rev. Lett. 96(12), 123901 (2006).
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B. Sepúlveda, A. Calle, L. M. Lechuga, and G. Armelles, “Highly sensitive detection of biomolecules with the magneto-optic surface-plasmon-resonance sensor,” Opt. Lett. 31(8), 1085–1087 (2006).
[Crossref] [PubMed]

Y. S. Joe, A. M. Satanin, and C. S. Kim, “Classical analogy of Fano resonances,” Phys. Scr. 74(2), 259–266 (2006).
[Crossref]

2005 (5)

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A. García-Martín, G. Armelles, and S. Pereira, “Light transport in photonic crystals composed of magneto-optically active materials,” Phys. Rev. B 71(20), 205116 (2005).
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A. Sundaramurthy, K. Crozier, G. Kino, D. Fromm, P. Schuck, and W. Moerner, “Field enhancement and gap-dependent resonance in a system of two opposing tip-to-tip Au nanotriangles,” Phys. Rev. B 72(16), 165409 (2005).
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P. Mühlschlegel, H.-J. Eisler, O. J. F. Martin, B. Hecht, and D. W. Pohl, “Resonant optical antennas,” Science 308(5728), 1607–1609 (2005).
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2004 (2)

D. P. Fromm, A. Sundaramurthy, P. J. Schuck, G. Kino, and W. E. Moerner, “Gap-dependent optical coupling of single «bowtie» nanoantennas resonant in the visible,” Nano Lett. 4(5), 957–961 (2004).
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S. Zou, N. Janel, and G. C. Schatz, “Silver nanoparticle array structures that produce remarkably narrow plasmon lineshapes,” J. Chem. Phys. 120(23), 10871–10875 (2004).
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2003 (3)

K.-H. Su, Q.-H. Wei, X. Zhang, J. J. Mock, D. R. Smith, and S. Schultz, “Interparticle coupling effects on plasmon resonances of nanogold particles,” Nano Lett. 3(8), 1087–1090 (2003).
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W. Rechberger, A. Hohenau, A. Leitner, J. R. Krenn, B. Lamprecht, and F. R. Aussenegg, “Optical properties of two interacting gold nanoparticles,” Opt. Commun. 220(1-3), 137–141 (2003).
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E. Prodan, C. Radloff, N. J. Halas, and P. Nordlander, “A hybridization model for the plasmon response of complex nanostructures,” Science 302(5644), 419–422 (2003).
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H. Fredriksson, Y. Alaverdyan, A. Dmitriev, C. Langhammer, D. S. Sutherland, M. Zäch, and B. Kasemo, “Hole–mask colloidal lithography,” Adv. Mater. 19(23), 4297–4302 (2007).
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J. N. Anker, W. P. Hall, O. Lyandres, N. C. Shah, J. Zhao, and R. P. Van Duyne, “Biosensing with plasmonic nanosensors,” Nat. Mater. 7(6), 442–453 (2008).
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G. Armelles, A. Cebollada, A. García-Martín, and M. U. González, “Magnetoplasmonics: combining magnetic and plasmonic functionalities,” Adv. Opt. Mater. 1(1), 10–35 (2013).
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A. García-Martín, G. Armelles, and S. Pereira, “Light transport in photonic crystals composed of magneto-optically active materials,” Phys. Rev. B 71(20), 205116 (2005).
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G. Armelles, A. Cebollada, A. García-Martín, and M. U. González, “Magnetoplasmonics: combining magnetic and plasmonic functionalities,” Adv. Opt. Mater. 1(1), 10–35 (2013).
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A. E. Cetin and H. Altug, “Fano resonant ring/disk plasmonic nanocavities on conducting substrates for advanced biosensing,” ACS Nano 6(11), 9989–9995 (2012).
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de Abajo, F. J. G.

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A. Dmitriev, T. Pakizeh, M. Käll, and D. S. Sutherland, “Gold-silica-gold nanosandwiches: tunable bimodal plasmonic resonators,” Small 3(2), 294–299 (2007).
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H. Fredriksson, Y. Alaverdyan, A. Dmitriev, C. Langhammer, D. S. Sutherland, M. Zäch, and B. Kasemo, “Hole–mask colloidal lithography,” Adv. Mater. 19(23), 4297–4302 (2007).
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Dregely, D.

Eisler, H.-J.

P. Mühlschlegel, H.-J. Eisler, O. J. F. Martin, B. Hecht, and D. W. Pohl, “Resonant optical antennas,” Science 308(5728), 1607–1609 (2005).
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Fan, J. A.

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S. E. Harris, J. E. Field, and A. Imamoğlu, “Nonlinear optical processes using electromagnetically induced transparency,” Phys. Rev. Lett. 64(10), 1107–1110 (1990).
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Y. Francescato, V. Giannini, and S. A. Maier, “Plasmonic systems unveiled by Fano resonances,” ACS Nano 6(2), 1830–1838 (2012).
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H. Fredriksson, Y. Alaverdyan, A. Dmitriev, C. Langhammer, D. S. Sutherland, M. Zäch, and B. Kasemo, “Hole–mask colloidal lithography,” Adv. Mater. 19(23), 4297–4302 (2007).
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Fromm, D. P.

Froufe-Pérez, L. S.

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García, F.

Garcia-Martin, A.

Garcia-Martin, J. M.

García-Martín, A.

G. Armelles, A. Cebollada, A. García-Martín, and M. U. González, “Magnetoplasmonics: combining magnetic and plasmonic functionalities,” Adv. Opt. Mater. 1(1), 10–35 (2013).
[Crossref]

A. García-Martín, G. Armelles, and S. Pereira, “Light transport in photonic crystals composed of magneto-optically active materials,” Phys. Rev. B 71(20), 205116 (2005).
[Crossref]

García-Martín, J. M.

Genov, D. A.

S. Zhang, D. A. Genov, Y. Wang, M. Liu, and X. Zhang, “Plasmon-induced transparency in metamaterials,” Phys. Rev. Lett. 101(4), 047401 (2008).
[Crossref] [PubMed]

Ghenuche, P.

Giannini, V.

Y. Francescato, V. Giannini, and S. A. Maier, “Plasmonic systems unveiled by Fano resonances,” ACS Nano 6(2), 1830–1838 (2012).
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Gómez Rivas, J.

Gómez-Medina, R.

González, M. U.

G. Armelles, A. Cebollada, A. García-Martín, and M. U. González, “Magnetoplasmonics: combining magnetic and plasmonic functionalities,” Adv. Opt. Mater. 1(1), 10–35 (2013).
[Crossref]

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Gopal, A. V.

Granpayeh, N.

Guzatov, D.

Halas, N. J.

E. Prodan, C. Radloff, N. J. Halas, and P. Nordlander, “A hybridization model for the plasmon response of complex nanostructures,” Science 302(5644), 419–422 (2003).
[Crossref] [PubMed]

Hall, W. P.

J. N. Anker, W. P. Hall, O. Lyandres, N. C. Shah, J. Zhao, and R. P. Van Duyne, “Biosensing with plasmonic nanosensors,” Nat. Mater. 7(6), 442–453 (2008).
[Crossref] [PubMed]

Hao, F.

Hao, Z.-H.

Harris, S. E.

S. E. Harris, J. E. Field, and A. Imamoğlu, “Nonlinear optical processes using electromagnetically induced transparency,” Phys. Rev. Lett. 64(10), 1107–1110 (1990).
[Crossref] [PubMed]

Hecht, B.

P. Mühlschlegel, H.-J. Eisler, O. J. F. Martin, B. Hecht, and D. W. Pohl, “Resonant optical antennas,” Science 308(5728), 1607–1609 (2005).
[Crossref] [PubMed]

Hentschel, M.

Hillenbrand, R.

Hohenau, A.

Huang, M.

Imamoglu, A.

S. E. Harris, J. E. Field, and A. Imamoğlu, “Nonlinear optical processes using electromagnetically induced transparency,” Phys. Rev. Lett. 64(10), 1107–1110 (1990).
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Janel, N.

S. Zou, N. Janel, and G. C. Schatz, “Silver nanoparticle array structures that produce remarkably narrow plasmon lineshapes,” J. Chem. Phys. 120(23), 10871–10875 (2004).
[Crossref] [PubMed]

Joe, Y. S.

Y. S. Joe, A. M. Satanin, and C. S. Kim, “Classical analogy of Fano resonances,” Phys. Scr. 74(2), 259–266 (2006).
[Crossref]

Jun, Y. C.

Käll, M.

A. Dmitriev, T. Pakizeh, M. Käll, and D. S. Sutherland, “Gold-silica-gold nanosandwiches: tunable bimodal plasmonic resonators,” Small 3(2), 294–299 (2007).
[Crossref] [PubMed]

Kasemo, B.

H. Fredriksson, Y. Alaverdyan, A. Dmitriev, C. Langhammer, D. S. Sutherland, M. Zäch, and B. Kasemo, “Hole–mask colloidal lithography,” Adv. Mater. 19(23), 4297–4302 (2007).
[Crossref]

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Kasture, S.

Kelley, B. K.

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Khanikaev, A. B.

Kim, C. S.

Y. S. Joe, A. M. Satanin, and C. S. Kim, “Classical analogy of Fano resonances,” Phys. Scr. 74(2), 259–266 (2006).
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Kotov, V. A.

Krenn, J. R.

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Langguth, L.

Langhammer, C.

C. Wadell, T. J. Antosiewicz, and C. Langhammer, “Optical absorption engineering in stacked plasmonic Au-SiO₂-Pd nanoantennas,” Nano Lett. 12(9), 4784–4790 (2012).
[Crossref] [PubMed]

H. Fredriksson, Y. Alaverdyan, A. Dmitriev, C. Langhammer, D. S. Sutherland, M. Zäch, and B. Kasemo, “Hole–mask colloidal lithography,” Adv. Mater. 19(23), 4297–4302 (2007).
[Crossref]

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Lechuga, L. M.

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S. Zhang, D. A. Genov, Y. Wang, M. Liu, and X. Zhang, “Plasmon-induced transparency in metamaterials,” Phys. Rev. Lett. 101(4), 047401 (2008).
[Crossref] [PubMed]

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Löffler, J. F.

Luk’yanchuk, B.

Lyandres, O.

J. N. Anker, W. P. Hall, O. Lyandres, N. C. Shah, J. Zhao, and R. P. Van Duyne, “Biosensing with plasmonic nanosensors,” Nat. Mater. 7(6), 442–453 (2008).
[Crossref] [PubMed]

Maier, S. A.

Y. Francescato, V. Giannini, and S. A. Maier, “Plasmonic systems unveiled by Fano resonances,” ACS Nano 6(2), 1830–1838 (2012).
[Crossref] [PubMed]

Mallouk, T.

Marinchio, H.

Martin, O. J. F.

B. Gallinet and O. J. F. Martin, “Influence of electromagnetic interactions on the line shape of plasmonic Fano resonances,” ACS Nano 5(11), 8999–9008 (2011).
[Crossref] [PubMed]

P. Mühlschlegel, H.-J. Eisler, O. J. F. Martin, B. Hecht, and D. W. Pohl, “Resonant optical antennas,” Science 308(5728), 1607–1609 (2005).
[Crossref] [PubMed]

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Mock, J. J.

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P. Mühlschlegel, H.-J. Eisler, O. J. F. Martin, B. Hecht, and D. W. Pohl, “Resonant optical antennas,” Science 308(5728), 1607–1609 (2005).
[Crossref] [PubMed]

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Nogués, J.

Nordlander, P.

E. Prodan, C. Radloff, N. J. Halas, and P. Nordlander, “A hybridization model for the plasmon response of complex nanostructures,” Science 302(5644), 419–422 (2003).
[Crossref] [PubMed]

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Pakizeh, T.

A. Dmitriev, T. Pakizeh, M. Käll, and D. S. Sutherland, “Gold-silica-gold nanosandwiches: tunable bimodal plasmonic resonators,” Small 3(2), 294–299 (2007).
[Crossref] [PubMed]

Papasimakis, N.

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A. García-Martín, G. Armelles, and S. Pereira, “Light transport in photonic crystals composed of magneto-optically active materials,” Phys. Rev. B 71(20), 205116 (2005).
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Pirzadeh, Z.

Pohl, D. W.

P. Mühlschlegel, H.-J. Eisler, O. J. F. Martin, B. Hecht, and D. W. Pohl, “Resonant optical antennas,” Science 308(5728), 1607–1609 (2005).
[Crossref] [PubMed]

Pohl, M.

Povinelli, M. L.

Prodan, E.

E. Prodan, C. Radloff, N. J. Halas, and P. Nordlander, “A hybridization model for the plasmon response of complex nanostructures,” Science 302(5644), 419–422 (2003).
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Quidant, R.

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E. Prodan, C. Radloff, N. J. Halas, and P. Nordlander, “A hybridization model for the plasmon response of complex nanostructures,” Science 302(5644), 419–422 (2003).
[Crossref] [PubMed]

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Richter, L. J.

Rodriguez, S. R. K.

Sáenz, J. J.

Saliba, M.

Sandhu, S.

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Y. S. Joe, A. M. Satanin, and C. S. Kim, “Classical analogy of Fano resonances,” Phys. Scr. 74(2), 259–266 (2006).
[Crossref]

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Schatz, G. C.

S. Zou, N. Janel, and G. C. Schatz, “Silver nanoparticle array structures that produce remarkably narrow plasmon lineshapes,” J. Chem. Phys. 120(23), 10871–10875 (2004).
[Crossref] [PubMed]

Schuck, P.

Schuck, P. J.

Schuller, J. A.

Schultz, S.

Sepúlveda, B.

Shah, N. C.

J. N. Anker, W. P. Hall, O. Lyandres, N. C. Shah, J. Zhao, and R. P. Van Duyne, “Biosensing with plasmonic nanosensors,” Nat. Mater. 7(6), 442–453 (2008).
[Crossref] [PubMed]

Shakya, J.

Shvets, G.

Smith, D. R.

Smythe, E. J.

Sobhani, H.

Solak, H. H.

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Soukoulis, C. M.

Steinle, T.

Stritzker, B.

Su, K.-H.

Sundaramurthy, A.

Sutherland, D. S.

A. Dmitriev, T. Pakizeh, M. Käll, and D. S. Sutherland, “Gold-silica-gold nanosandwiches: tunable bimodal plasmonic resonators,” Small 3(2), 294–299 (2007).
[Crossref] [PubMed]

H. Fredriksson, Y. Alaverdyan, A. Dmitriev, C. Langhammer, D. S. Sutherland, M. Zäch, and B. Kasemo, “Hole–mask colloidal lithography,” Adv. Mater. 19(23), 4297–4302 (2007).
[Crossref]

Taminiau, T. H.

Temnov, V. V.

Thomay, T.

Torrado, J. F.

Van Dorpe, P.

Van Duyne, R. P.

J. N. Anker, W. P. Hall, O. Lyandres, N. C. Shah, J. Zhao, and R. P. Van Duyne, “Biosensing with plasmonic nanosensors,” Nat. Mater. 7(6), 442–453 (2008).
[Crossref] [PubMed]

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Vavassori, P.

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Vogelgesang, R.

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C. Wadell, T. J. Antosiewicz, and C. Langhammer, “Optical absorption engineering in stacked plasmonic Au-SiO₂-Pd nanoantennas,” Nano Lett. 12(9), 4784–4790 (2012).
[Crossref] [PubMed]

Wang, Q.-Q.

Wang, Y.

S. Zhang, D. A. Genov, Y. Wang, M. Liu, and X. Zhang, “Plasmon-induced transparency in metamaterials,” Phys. Rev. Lett. 101(4), 047401 (2008).
[Crossref] [PubMed]

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H. Fredriksson, Y. Alaverdyan, A. Dmitriev, C. Langhammer, D. S. Sutherland, M. Zäch, and B. Kasemo, “Hole–mask colloidal lithography,” Adv. Mater. 19(23), 4297–4302 (2007).
[Crossref]

Zhang, L.-H.

Zhang, S.

S. Zhang, D. A. Genov, Y. Wang, M. Liu, and X. Zhang, “Plasmon-induced transparency in metamaterials,” Phys. Rev. Lett. 101(4), 047401 (2008).
[Crossref] [PubMed]

Zhang, X.

S. Zhang, D. A. Genov, Y. Wang, M. Liu, and X. Zhang, “Plasmon-induced transparency in metamaterials,” Phys. Rev. Lett. 101(4), 047401 (2008).
[Crossref] [PubMed]

Zhang, Y.

Zhang, Z.-S.

Zhao, J.

J. N. Anker, W. P. Hall, O. Lyandres, N. C. Shah, J. Zhao, and R. P. Van Duyne, “Biosensing with plasmonic nanosensors,” Nat. Mater. 7(6), 442–453 (2008).
[Crossref] [PubMed]

Zheludev, N. I.

Zhou, J. F.

Zou, S.

S. Zou, N. Janel, and G. C. Schatz, “Silver nanoparticle array structures that produce remarkably narrow plasmon lineshapes,” J. Chem. Phys. 120(23), 10871–10875 (2004).
[Crossref] [PubMed]

Zvezdin, A. K.

ACS Nano (5)

Y. Francescato, V. Giannini, and S. A. Maier, “Plasmonic systems unveiled by Fano resonances,” ACS Nano 6(2), 1830–1838 (2012).
[Crossref] [PubMed]

B. Gallinet and O. J. F. Martin, “Influence of electromagnetic interactions on the line shape of plasmonic Fano resonances,” ACS Nano 5(11), 8999–9008 (2011).
[Crossref] [PubMed]

A. E. Cetin and H. Altug, “Fano resonant ring/disk plasmonic nanocavities on conducting substrates for advanced biosensing,” ACS Nano 6(11), 9989–9995 (2012).
[Crossref] [PubMed]

Adv. Mater. (2)

H. Fredriksson, Y. Alaverdyan, A. Dmitriev, C. Langhammer, D. S. Sutherland, M. Zäch, and B. Kasemo, “Hole–mask colloidal lithography,” Adv. Mater. 19(23), 4297–4302 (2007).
[Crossref]

Adv. Opt. Mater. (1)

G. Armelles, A. Cebollada, A. García-Martín, and M. U. González, “Magnetoplasmonics: combining magnetic and plasmonic functionalities,” Adv. Opt. Mater. 1(1), 10–35 (2013).
[Crossref]

IEEE J. Sel. Top. Quantum Electron. (1)

J. Chem. Phys. (1)

S. Zou, N. Janel, and G. C. Schatz, “Silver nanoparticle array structures that produce remarkably narrow plasmon lineshapes,” J. Chem. Phys. 120(23), 10871–10875 (2004).
[Crossref] [PubMed]

J. Opt. Soc. Am. B (1)

J. Phys. Chem. C (1)

Nano Lett. (7)

C. Wadell, T. J. Antosiewicz, and C. Langhammer, “Optical absorption engineering in stacked plasmonic Au-SiO₂-Pd nanoantennas,” Nano Lett. 12(9), 4784–4790 (2012).
[Crossref] [PubMed]

Nat Commun (1)

Nat. Mater. (5)

J. N. Anker, W. P. Hall, O. Lyandres, N. C. Shah, J. Zhao, and R. P. Van Duyne, “Biosensing with plasmonic nanosensors,” Nat. Mater. 7(6), 442–453 (2008).
[Crossref] [PubMed]

Nat. Nanotechnol. (1)

Nat. Photonics (1)

Opt. Commun. (1)

Opt. Express (2)

Opt. Lett. (3)

Phys. Rev. B (4)

A. García-Martín, G. Armelles, and S. Pereira, “Light transport in photonic crystals composed of magneto-optically active materials,” Phys. Rev. B 71(20), 205116 (2005).
[Crossref]

Phys. Rev. Lett. (7)

S. E. Harris, J. E. Field, and A. Imamoğlu, “Nonlinear optical processes using electromagnetically induced transparency,” Phys. Rev. Lett. 64(10), 1107–1110 (1990).
[Crossref] [PubMed]

S. Zhang, D. A. Genov, Y. Wang, M. Liu, and X. Zhang, “Plasmon-induced transparency in metamaterials,” Phys. Rev. Lett. 101(4), 047401 (2008).
[Crossref] [PubMed]

B. Auguié and W. L. Barnes, “Collective resonances in gold nanoparticle arrays,” Phys. Rev. Lett. 101(14), 143902 (2008).
[Crossref] [PubMed]

Phys. Scr. (1)

Y. S. Joe, A. M. Satanin, and C. S. Kim, “Classical analogy of Fano resonances,” Phys. Scr. 74(2), 259–266 (2006).
[Crossref]

Proc. Natl. Acad. Sci. U.S.A. (1)

Science (2)

E. Prodan, C. Radloff, N. J. Halas, and P. Nordlander, “A hybridization model for the plasmon response of complex nanostructures,” Science 302(5644), 419–422 (2003).
[Crossref] [PubMed]

P. Mühlschlegel, H.-J. Eisler, O. J. F. Martin, B. Hecht, and D. W. Pohl, “Resonant optical antennas,” Science 308(5728), 1607–1609 (2005).
[Crossref] [PubMed]

Small (2)

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[Crossref] [PubMed]

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Supplementary Material (2)

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Fig. 1 (a) Spring model representing a two coupled masses system excited by an harmonic force, F(t), along x axis. Left side: uncharged masses. Right side-(

Media 1

): one of the masses (blue) is charged (q) and a static magnetic field (B) is applied along the z direction, inducing a Lorentz force, F_l(t), along the y direction. The y-movement is transferred to the other mass through the coupling. (b) Two interacting electric dipoles, representing two metallic disks, excited by an incident beam polarized along the x axis. Left side: No disk has magneto-optical activity and the reflected (E_r) and transmitted (E_t) light have the same polarization direction than the incident (E_i) light. Right side: one of the disks (blue) has magneto-optical activity and a static magnetic field (B) applied along the z direction induces a rotation of its electric dipole, which is transferred to the other dipole through the interaction. The rotation modifies the polarization direction of the reflected (E_r) and transmitted (E_t) light.

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Fig. 2 (a) Schematic drawing of the nanoresonators composed of a purely plasmonic Au disk and a magnetoplasmonic Au/Co superlattice disk separated by a dielectric spacer. (b) Polar Kerr loop of a characteristic sample. The presence of multiple Co/Au interfaces reduces the value of the magnetic field needed to saturate the nanodisks in the direction perpendicular to the sample plane. (c), (d) Cross section and planar view SEM pictures, respectively, of a representative sample. The images show the homogeneous and random distribution of nanoresonators and their truncated conical shape and internal structure.

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Fig. 3 (a) Extinction and (b) MO activity spectra of the nanoresonators as a function of SiO₂ thickness. The different dashed horizontal lines indicate the zero value for each spectrum above the line. The 3D graphs on top of each panel show the results obtained from theoretical calculations of the same structures. The blue, green and red diamonds appearing in the experimental MO response for 20 nm SiO₂ correspond to the spectral positions where the E_z field distributions are calculated [see Fig. 4].

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Fig. 4 (a) Calculated near field intensity of the E_z component for a nanoresonator with 20 nm SiO₂ spacer in two planes above the top disk and below the bottom one, with the incident field polarized along the x direction and in the absence of an external magnetic field. This distribution reflects the excitation of two dipoles along the x direction. The insets indicate the corresponding charges and dipole orientations (indicated by the black arrows) according to the E_z distribution for the different cases. The red (blue) arrows in the insets represent the positive (negative) values of the Ez field component. (b) Difference of the E_z components for magnetic saturation along opposite directions in the same planes and for the same structure. This difference accounts for the effect of the applied magnetic field: The appearance of a dipole along the y direction for both the magnetoplasmonic (intrinsic dipole) and the plasmonic (induced dipole) disks. In both cases, the components for three different wavelengths labelled as diamonds in Fig. 3 are shown.

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Fig. 5 Fano resonance in the magneto-optical activity. (a) Experimental spectra of the MO activity for the structures with 20 nm and 50 nm SiO₂ spacer, corresponding to interacting and non-interacting situations, respectively. For the interacting situation a clear Fano resonance shape is observed. The inset shows the difference between the two spectra, resulting in a narrow peak. (b) Theoretical MO activity spectra obtained for a structure with 20nm SiO₂ spacer and for the same structure but without the upper metallic disk. The inset shows the MO spectra obtained using the simple point dipole model.

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Fig. 6 Oscillation amplitude as a function of the frequency of masses 1 (uncharged) and 2 (charged) along x- (left panel) and y- (right panel) direction by using a simple spring-mass model. Inset: Frame of a video showing schematically the evolution with the frequency of the masses’ oscillation for frequency values around the minimum in x-amplitude for the charged mass 2 (in the video, the y-amplitude has been multiplied by a factor 10, and the frequency has been scaled as ω_vid = (1 + (ω-0.93) × 50)ω₂ for clarity in the visualization) (Media 2).

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Fig. 7 Wavelength dependence of the normalized dipole magnitudes along the x- (left panel) and y- (right panel) directions obtained using a point dipole model.

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Equations (19)

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{\begin{cases} p_{1 x} = \frac{E_{0, 1 x}}{D} α_{1} [1 + G α_{2 x x} (e^{i δ} - G α_{1}) - G^{3} α_{1} (α_{2 x x}^{2} + α_{2 x y}^{2}) e^{i δ}] \\ p_{1 y} = - \frac{E_{0, 1 x}}{D} G α_{1} α_{2 x y} [e^{i δ} + G α_{1}] \\ p_{2 x} = \frac{E_{0, 1 x}}{D} [α_{2 x x} - G^{2} α_{1} (α_{2 x x}^{2} + α_{2 x y}^{2})] [e^{i δ} + G α_{1}] \\ p_{2 y} = - \frac{E_{0, 1 x}}{D} α_{2 x y} [e^{i δ} + G α_{1}] \end{cases},

\begin{array}{l} m_{1} {\ddot{r}}_{1} = F_{1} - k_{1} r_{1} - k_{12} (r_{1} - r_{2}) - B_{1} {\dot{r}}_{1} \\ m_{2} {\ddot{r}}_{2} = F_{2} - k_{2} r_{2} - k_{12} (r_{2} - r_{1}) - B_{2} {\dot{r}}_{2} \end{array},

B_{i} = b_{i} + F_{l}^{i} = [\begin{matrix} b_{i} & 0 \\ 0 & b_{i} \end{matrix}] + [\begin{matrix} 0 & - q B_{i} \\ q B_{i} & 0 \end{matrix}]

F_{l}^{i} = q B_{i} [\begin{matrix} 0 & 1 \\ - 1 & 0 \end{matrix}] (\begin{matrix} {\dot{r}}_{x} \\ {\dot{r}}_{y} \end{matrix}) .

\begin{array}{l} ω_{i}^{2} \equiv k_{i} / m \\ ω_{12}^{2} \equiv k_{12} / m \\ Γ_{i} \equiv B_{i} / m \equiv (\begin{matrix} γ_{i} & - ω_{c, i} \\ ω_{c, i} & γ_{i} \end{matrix}) \end{array}

\begin{array}{l} - ℱ_{1} = (ω^{2} - ω_{1}^{2} + i ω Γ_{1} - ω_{12}^{2}) r_{1} + (ω_{12}^{2}) r_{2} \\ - ℱ_{2} = (ω^{2} - ω_{2}^{2} + i ω Γ_{2} - ω_{12}^{2}) r_{2} + (ω_{12}^{2}) r_{1} \end{array}

M (\begin{matrix} r_{1} \\ r_{2} \end{matrix}) \equiv [\begin{matrix} ((Ω_{1}^{2} - ω_{12}^{2}) I + ω ω_{c, 1} σ_{2}) & ω_{12}^{2} I \\ ω_{12}^{2} I & ((Ω_{2}^{2} - ω_{12}^{2}) I + ω ω_{c, 2} σ_{2}) \end{matrix}] (\begin{matrix} r_{1} \\ r_{2} \end{matrix}) = (\begin{matrix} - ℱ_{1} \\ - ℱ_{2} \end{matrix}),

{\begin{cases} x_{1} = \frac{- ℱ_{x}}{D} [[Ω_{1}^{2} Ω_{2}^{2} - ω_{12}^{2} (Ω_{1}^{2} + Ω_{2}^{2})] (Ω_{2}^{2} - 2 ω_{12}^{2}) - ω^{2} ω_{c}^{2} (Ω_{1}^{2} - ω_{12}^{2})] \\ y_{1} = \frac{- ℱ_{x}}{D} [i ω ω_{c} ω_{12}^{2} (Ω_{1}^{2} - 2 ω_{12}^{2})] \\ x_{2} = \frac{- ℱ_{x}}{D} [[Ω_{1}^{2} Ω_{2}^{2} - ω_{12}^{2} (Ω_{1}^{2} + Ω_{2}^{2})] (Ω_{1}^{2} - 2 ω_{12}^{2})] \\ y_{2} = \frac{- ℱ_{x}}{D} [- i ω ω_{c} (Ω_{1}^{2} - ω_{12}^{2}) (Ω_{1}^{2} - 2 ω_{12}^{2})] \end{cases},

[\begin{matrix} a & 0 & c & 0 \\ 0 & a & 0 & c \\ c & 0 & d & - b \\ 0 & c & b & d \end{matrix}] [\begin{matrix} x_{1} \\ y_{1} \\ x_{2} \\ y_{2} \end{matrix}] = A [\begin{matrix} 1 \\ 0 \\ 1 \\ 0 \end{matrix}] .

[\begin{matrix} x_{1} \\ y_{1} \\ x_{2} \\ y_{2} \end{matrix}] = \frac{A}{D} [\begin{matrix} a d^{2} - d c^{2} + b^{2} a & b c^{2} & c^{3} - d c a & - b c a \\ - b c^{2} & a d^{2} - d c^{2} + b^{2} a & b c a & c^{3} - d c a \\ c^{3} - d c a & - b c a & d a^{2} - c^{2} a & a^{2} b \\ b c a & c^{3} - d c a & - b a^{2} & d a^{2} - c^{2} a \end{matrix}] [\begin{matrix} 1 \\ 0 \\ 1 \\ 0 \end{matrix}],

{\begin{cases} x_{1} = \frac{A}{D} [(c^{2} - a d) (c - d) + b^{2} a] \\ y_{1} = \frac{A}{D} [- b c (c - a)] \\ x_{2} = \frac{A}{D} [(c^{2} - a d) (c - a)] \\ y_{2} = \frac{A}{D} [b a (c - a)] \end{cases} .

α_{0} = V \frac{ε + I}{I + L (ε - I)}, \tilde{α} = \frac{α_{0}}{I - i \frac{k^{3}}{6 π} α_{0}},

G (r, r^{'}) = \frac{e^{i k R}}{4 π R} {\frac{{(k R)}^{2} + i k R - 1}{{(k R)}^{2}} I + \frac{- {(k R)}^{2} - 3 i k R + 3}{{(k R)}^{2}} \frac{R \otimes R}{R^{2}}} .

E_{i} = E_{0, i} + \sum_{i \neq j}^{N} G (r_{i}, r_{j}) p_{j} .

α_{i} = [\begin{matrix} α_{i, x x} & α_{i, x y} & 0 \\ - α_{i, x y} & α_{i, x x} & 0 \\ 0 & 0 & α_{i, z z} \end{matrix}],

G (r_{1}, r_{2}) = G (r_{2}, r_{1}) = G I = \frac{e^{i k d}}{4 π d} \frac{{(k d)}^{2} + i k d - 1}{{(k d)}^{2}} I,

{\begin{cases} α_{1}^{- 1} p_{1} = E_{0, 1} + G p_{2} = E_{0, 1 x} + G p_{2} \\ α_{2}^{- 1} p_{2} = E_{0, 2} + G p_{1} = E_{0, 1 x} e^{i δ} + G p_{1} \end{cases}

M (\begin{matrix} p_{1} \\ p_{2} \end{matrix}) \equiv [\begin{matrix} α_{1}^{- 1} & - G I \\ - G I & α_{2}^{- 1} \end{matrix}] (\begin{matrix} p_{1} \\ p_{2} \end{matrix}) = (\begin{matrix} E_{0, 1} \\ E_{0, 1} e^{i δ} \end{matrix}),

{\begin{cases} p_{1 x} = \frac{E_{0, 1 x}}{D} α_{1} [1 + G α_{2 x x} (e^{i δ} - G α_{1}) - G^{3} α_{1} (α_{2 x x}^{2} + α_{2 x y}^{2}) e^{i δ}] \\ p_{1 y} = - \frac{E_{0, 1 x}}{D} G α_{1} α_{2 x y} [e^{i δ} + G α_{1}] \\ p_{2 x} = \frac{E_{0, 1 x}}{D} [α_{2 x x} - G^{2} α_{1} (α_{2 x x}^{2} + α_{2 x y}^{2})] [e^{i δ} + G α_{1}] \\ p_{2 y} = - \frac{E_{0, 1 x}}{D} α_{2 x y} [e^{i δ} + G α_{1}] \end{cases},