Fano-like resonance in symmetry-broken gold nanotube dimer

DaJian Wu; ShuMin Jiang; Ying Cheng; XiaoJun Liu

doi:10.1364/OE.20.026559

Fano-like resonance in symmetry-broken gold nanotube dimer

DaJian Wu, ShuMin Jiang, Ying Cheng, and XiaoJun Liu

Optics Express
Vol. 20,
Issue 24,
pp. 26559-26567
(2012)
•https://doi.org/10.1364/OE.20.026559

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DaJian Wu, ShuMin Jiang, Ying Cheng, and XiaoJun Liu, "Fano-like resonance in symmetry-broken gold nanotube dimer," Opt. Express 20, 26559-26567 (2012)

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Related Topics
Table of Contents Category
- Optics at Surfaces
Optics & Photonics Topics
?

The topics in this list come from the OSA Optics and Photonics Topics applied to this article.
Previously assigned OCIS codes
- Optical properties (160.4760)
- Surface plasmons (240.6680)
- Nanophotonics and photonic crystals (350.4238)
- Resonance (260.5740)

About this Article
History
- Original Manuscript: August 30, 2012
- Revised Manuscript: November 6, 2012
- Manuscript Accepted: November 6, 2012
- Published: November 12, 2012

Accessible

Open Access

Abstract

The influences of the symmetry-breaking on the plasmon resonance couplings in the isolated gold nanotube and the gold nanotube dimer have been investigated by means of the finite element method. It is found that the core offset of gold nanotubes leads to the red-shifts of the low energy modes and the enhanced near-field on the thin shell side of the symmetry-broken gold nanotube (SBGNT). In the weak coupling model of the SBGNT dimer, the interference of the bonding octupole mode of the dimer with the dipole modes causes a strong Fano-like resonance in scattering spectrum. The Fano dip shows a red-shift and becomes deep with the increase of the offset-value. In the strong coupling model of the SBGNT dimer, the coupling between two SBGNTs induces giant electric field enhancement at the gap of the dimer, which is much larger than that in the symmetry gold nanotube dimer. The SBGNT with larger offset-value exhibits stronger near-field at the “hot spot”.

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D. C. Marinica, A. K. Kazansky, P. Nordlander, J. Aizpurua, and A. G. Borisov, “Quantum plasmonics: nonlinear effects in the field enhancement of a plasmonic nanoparticle dimer,” Nano Lett. 12(3), 1333–1339 (2012).
[Crossref] [PubMed]

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[Crossref] [PubMed]

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[Crossref] [PubMed]

2011 (11)

H. Q. Xu, H. J. Li, Z. M. Liu, S. X. Xie, X. Zhou, X. Peng, and X. K. Xu, “Effects of symmetry breaking on plasmon resonance in a noncoaxial nanotube and nanotube dimer,” J. Opt. Soc. Am. A 28(8), 1662–1667 (2011).
[Crossref] [PubMed]

M. Wang, M. Cao, X. Chen, and N. Gu, “Subradiant plasmon modes in multilayer metal–dielectric nanoshells,” J. Phys. Chem. C 115(43), 20920–20925 (2011).
[Crossref]

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), http://www.opticsinfobase.org/ol/abstract.cfm?URI=ol-36-9-1542 .
[Crossref] [PubMed]

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[Crossref] [PubMed]

N. J. Halas, S. Lal, W. S. Chang, S. Link, and P. Nordlander, “Plasmons in strongly coupled metallic nanostructures,” Chem. Rev. 111(6), 3913–3961 (2011).
[Crossref] [PubMed]

M. G. Blaber and G. C. Schatz, “Extending SERS into the infrared with gold nanosphere dimers,” Chem. Commun. (Camb.) 47(13), 3769–3771 (2011).
[Crossref] [PubMed]

Y. Y. Rao, Q. Tao, M. An, C. H. Rong, J. Dong, Y. R. Dai, and W. P. Qian, “Novel and simple route to fabricate 2D ordered gold nanobowl arrays based on 3D colloidal crystals,” Langmuir 27(21), 13308–13313 (2011).
[Crossref] [PubMed]

O. Peña-Rodríguez and U. Pal, “Enhanced plasmonic behavior of incomplete nanoshells: effect of local field irregularities on the far-field optical response,” J. Phys. Chem. C 115(45), 22271–22275 (2011).
[Crossref]

L. F. Niu, J. B. Zhang, Y. H. Fu, S. Kulkarni, and B. Luky Anchuk, “Fano resonance in dual-disk ring plasmonic nanostructures,” Opt. Express 19(23), 22974–22981 (2011), http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-19-23-22974 .
[Crossref] [PubMed]

O. Peña-Rodríguez and U. Pal, “Au@Ag core-shell nanoparticles: efficient all-plasmonic Fano-resonance generators,” Nanoscale 3(9), 3609–3612 (2011).
[Crossref] [PubMed]

Z. Y. Fang, J. Y. Cai, Z. B. Yan, P. Nordlander, N. J. Halas, and X. Zhu, “Removing a wedge from a metallic nanodisk reveals a Fano resonance,” Nano Lett. 11(10), 4475–4479 (2011).
[Crossref] [PubMed]

2010 (5)

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]

S. Mukherjee, H. Sobhani, J. B. Lassiter, R. Bardhan, P. Nordlander, and N. J. Halas, “Fanoshells: nanoparticles with built-in Fano resonances,” Nano Lett. 10(7), 2694–2701 (2010).
[Crossref] [PubMed]

B. F. Yun, Z. Y. Wang, G. H. Hu, and Y. P. Cui, “Theoretical studies on the near field properties of non-concentric core–shell nanoparticle dimers,” Opt. Commun. 283(14), 2947–2952 (2010).
[Crossref]

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]

J. A. Fan, C. Wu, K. Bao, J. Bao, R. Bardhan, N. J. Halas, V. N. Manoharan, P. Nordlander, G. Shvets, and F. Capasso, “Self-assembled plasmonic nanoparticle clusters,” Science 328(5982), 1135–1138 (2010).
[Crossref] [PubMed]

2009 (2)

N. A. Mirin, K. Bao, and P. Nordlander, “Fano resonances in plasmonic nanoparticle aggregates,” J. Phys. Chem. A 113(16), 4028–4034 (2009).
[Crossref] [PubMed]

F. Hao, P. Nordlander, Y. Sonnefraud, P. Van Dorpe, and S. A. Maier, “Tunability of subradiant dipolar and Fano-type plasmon resonances in metallic ring/disk cavities: implications for nanoscale optical sensing,” ACS Nano 3(3), 643–652 (2009).
[Crossref] [PubMed]

2008 (4)

F. Hao, Y. Sonnefraud, P. Van Dorpe, S. A. Maier, N. J. Halas, and P. Nordlander, “Symmetry breaking in plasmonic nanocavities: subradiant LSPR sensing and a tunable Fano resonance,” Nano Lett. 8(11), 3983–3988 (2008).
[Crossref] [PubMed]

J. B. Lassiter, J. Aizpurua, L. I. Hernandez, D. W. Brandl, I. Romero, S. Lal, J. H. Hafner, P. Nordlander, and N. J. Halas, “Close encounters between two nanoshells,” Nano Lett. 8(4), 1212–1218 (2008).
[Crossref] [PubMed]

M. W. Knight and N. J. Halas, “Nanoshells to nanoeggs to nanocups: optical properties of reduced symmetry core-shell nanoparticles beyond the quasistatic limit,” New J. Phys. 10(10), 105006 (2008).
[Crossref]

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]

2006 (2)

Y. P. Wu and P. Nordlander, “Plasmon hybridization in nanoshells with a nonconcentric core,” J. Chem. Phys. 125(12), 124708 (2006).
[Crossref] [PubMed]

H. Wang, Y. P. Wu, B. Lassiter, C. L. Nehl, J. H. Hafner, P. Nordlander, and N. J. Halas, “Symmetry breaking in individual plasmonic nanoparticles,” Proc. Natl. Acad. Sci. U.S.A. 103(29), 10856–10860 (2006).
[Crossref] [PubMed]

2004 (2)

P. Nordlander, C. Oubre, E. Prodan, K. Li, and M. Stockman, “Plasmon hybridization in nanoparticle dimers,” Nano Lett. 4(5), 899–903 (2004).
[Crossref]

E. Prodan and P. Nordlander, “Plasmon hybridization in spherical nanoparticles,” J. Chem. Phys. 120(11), 5444–5454 (2004).
[Crossref] [PubMed]

2003 (1)

K. L. Kelly, E. Coronado, L. L. Zhao, and G. C. Schatz, “The Optical properties of metal nanoparticles: the influence of size, shape, and dielectric environment,” J. Phys. Chem. B 107(3), 668–677 (2003).
[Crossref]

1972 (1)

P. B. Johnson and R. W. Christy, “Optical constants of the noble metals,” Phys. Rev. B 6(12), 4370–4379 (1972).
[Crossref]

Aizpurua, J.

An, M.

Bao, J.

Bao, K.

N. A. Mirin, K. Bao, and P. Nordlander, “Fano resonances in plasmonic nanoparticle aggregates,” J. Phys. Chem. A 113(16), 4028–4034 (2009).
[Crossref] [PubMed]

Bardhan, R.

Blaber, M. G.

M. G. Blaber and G. C. Schatz, “Extending SERS into the infrared with gold nanosphere dimers,” Chem. Commun. (Camb.) 47(13), 3769–3771 (2011).
[Crossref] [PubMed]

Borisov, A. G.

Brandl, D. W.

Brown, L. V.

Cai, J. Y.

Cao, M.

M. Wang, M. Cao, X. Chen, and N. Gu, “Subradiant plasmon modes in multilayer metal–dielectric nanoshells,” J. Phys. Chem. C 115(43), 20920–20925 (2011).
[Crossref]

Capasso, F.

Chang, W. S.

N. J. Halas, S. Lal, W. S. Chang, S. Link, and P. Nordlander, “Plasmons in strongly coupled metallic nanostructures,” Chem. Rev. 111(6), 3913–3961 (2011).
[Crossref] [PubMed]

Chen, X.

M. Wang, M. Cao, X. Chen, and N. Gu, “Subradiant plasmon modes in multilayer metal–dielectric nanoshells,” J. Phys. Chem. C 115(43), 20920–20925 (2011).
[Crossref]

Chong, C. T.

Christy, R. W.

P. B. Johnson and R. W. Christy, “Optical constants of the noble metals,” Phys. Rev. B 6(12), 4370–4379 (1972).
[Crossref]

Coronado, E.

Cui, Y. P.

Dai, Y. R.

Dong, J.

Fan, J. A.

Fang, Z. Y.

Fu, Y. H.

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]

Giessen, H.

Gu, N.

M. Wang, M. Cao, X. Chen, and N. Gu, “Subradiant plasmon modes in multilayer metal–dielectric nanoshells,” J. Phys. Chem. C 115(43), 20920–20925 (2011).
[Crossref]

Hafner, J. H.

Halas, N. J.

N. J. Halas, S. Lal, W. S. Chang, S. Link, and P. Nordlander, “Plasmons in strongly coupled metallic nanostructures,” Chem. Rev. 111(6), 3913–3961 (2011).
[Crossref] [PubMed]

Hao, F.

Hao, Z. H.

Hernandez, L. I.

Hu, G. H.

Jiang, C. Y.

Jiang, S. M.

D. J. Wu, S. M. Jiang, and X. J. Liu, “A tunable Fano resonance in silver nanoshell with a spherically anisotropic core,” J. Chem. Phys. 136(3), 034502 (2012).
[Crossref] [PubMed]

Johnson, P. B.

P. B. Johnson and R. W. Christy, “Optical constants of the noble metals,” Phys. Rev. B 6(12), 4370–4379 (1972).
[Crossref]

Kazansky, A. K.

Kelly, K. L.

Knight, M. W.

Kulkarni, S.

Lal, S.

N. J. Halas, S. Lal, W. S. Chang, S. Link, and P. Nordlander, “Plasmons in strongly coupled metallic nanostructures,” Chem. Rev. 111(6), 3913–3961 (2011).
[Crossref] [PubMed]

Lassiter, B.

Lassiter, J. B.

Li, H. J.

Li, K.

P. Nordlander, C. Oubre, E. Prodan, K. Li, and M. Stockman, “Plasmon hybridization in nanoparticle dimers,” Nano Lett. 4(5), 899–903 (2004).
[Crossref]

Li, Q. Q.

Link, S.

N. J. Halas, S. Lal, W. S. Chang, S. Link, and P. Nordlander, “Plasmons in strongly coupled metallic nanostructures,” Chem. Rev. 111(6), 3913–3961 (2011).
[Crossref] [PubMed]

Liu, M.

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]

Liu, X. J.

D. J. Wu, S. M. Jiang, and X. J. Liu, “A tunable Fano resonance in silver nanoshell with a spherically anisotropic core,” J. Chem. Phys. 136(3), 034502 (2012).
[Crossref] [PubMed]

Liu, Z. M.

Luk’yanchuk, B.

Luky Anchuk, B.

Ma, X. Y.

Maier, S. A.

Manoharan, V. N.

Marinica, D. C.

Mielczarek, W. S.

Mirin, N. A.

N. A. Mirin, K. Bao, and P. Nordlander, “Fano resonances in plasmonic nanoparticle aggregates,” J. Phys. Chem. A 113(16), 4028–4034 (2009).
[Crossref] [PubMed]

Mukherjee, S.

Nehl, C. L.

Niu, L. F.

Nordlander, P.

N. J. Halas, S. Lal, W. S. Chang, S. Link, and P. Nordlander, “Plasmons in strongly coupled metallic nanostructures,” Chem. Rev. 111(6), 3913–3961 (2011).
[Crossref] [PubMed]

N. A. Mirin, K. Bao, and P. Nordlander, “Fano resonances in plasmonic nanoparticle aggregates,” J. Phys. Chem. A 113(16), 4028–4034 (2009).
[Crossref] [PubMed]

Y. P. Wu and P. Nordlander, “Plasmon hybridization in nanoshells with a nonconcentric core,” J. Chem. Phys. 125(12), 124708 (2006).
[Crossref] [PubMed]

P. Nordlander, C. Oubre, E. Prodan, K. Li, and M. Stockman, “Plasmon hybridization in nanoparticle dimers,” Nano Lett. 4(5), 899–903 (2004).
[Crossref]

E. Prodan and P. Nordlander, “Plasmon hybridization in spherical nanoparticles,” J. Chem. Phys. 120(11), 5444–5454 (2004).
[Crossref] [PubMed]

Oubre, C.

P. Nordlander, C. Oubre, E. Prodan, K. Li, and M. Stockman, “Plasmon hybridization in nanoparticle dimers,” Nano Lett. 4(5), 899–903 (2004).
[Crossref]

Pal, U.

O. Peña-Rodríguez and U. Pal, “Au@Ag core-shell nanoparticles: efficient all-plasmonic Fano-resonance generators,” Nanoscale 3(9), 3609–3612 (2011).
[Crossref] [PubMed]

Peña-Rodríguez, O.

O. Peña-Rodríguez and U. Pal, “Au@Ag core-shell nanoparticles: efficient all-plasmonic Fano-resonance generators,” Nanoscale 3(9), 3609–3612 (2011).
[Crossref] [PubMed]

Peng, X.

Prodan, E.

P. Nordlander, C. Oubre, E. Prodan, K. Li, and M. Stockman, “Plasmon hybridization in nanoparticle dimers,” Nano Lett. 4(5), 899–903 (2004).
[Crossref]

E. Prodan and P. Nordlander, “Plasmon hybridization in spherical nanoparticles,” J. Chem. Phys. 120(11), 5444–5454 (2004).
[Crossref] [PubMed]

Qian, W. P.

Rao, Y. Y.

Romero, I.

Rong, C. H.

Schatz, G. C.

M. G. Blaber and G. C. Schatz, “Extending SERS into the infrared with gold nanosphere dimers,” Chem. Commun. (Camb.) 47(13), 3769–3771 (2011).
[Crossref] [PubMed]

Shvets, G.

Sobhani, H.

Sonnefraud, Y.

Stockman, M.

P. Nordlander, C. Oubre, E. Prodan, K. Li, and M. Stockman, “Plasmon hybridization in nanoparticle dimers,” Nano Lett. 4(5), 899–903 (2004).
[Crossref]

Su, Q. Q.

Tao, Q.

Van Dorpe, P.

Wang, H.

Wang, M.

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Fig. 1 Scheme of the dimer of infinitely long noncoaxial nanotube.

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Fig. 2 (a) Far-field spectra of the coaxial gold nanotube. (b) Far-field spectra of the SBGNT with the offset-value of 23 nm. (c) Scattering spectra of the SBGNTs with various offset-values.

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Fig. 3 E-field enhancement distributions of SBGNT at the wavelengths of (a) 880 nm (dipole peak), (b) 820 nm (quadrupole peak), and (c) 648 nm (octupole peak). (d) Variations of the near-field enhancements in the gold nanotube and SBGNT.

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Fig. 4 Far-field spectra of (a) the model I, (b) the model II, and (c) the model III. (d) Variations of the E-field enhancement at C point shown in Fig. 1 for the model I, II, and III.

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Fig. 5 E-field enhancement distributions of the SBGNT dimers at the wavelengths of (a) 675 nm, (b) 765 nm (Fano minimum), (c) 827 nm (subradiant mode), and (d) 955 nm. Surface charge distributions of the SBGNT dimers at the wavelengths of (e) 675 nm, (f) 765 nm, (g) 827 nm, and (h) 955 nm.

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Fig. 6 (a) Scattering spectra of the model II with various offset-values. (b) E-field enhancements at C point shown in Fig. 1 for the model III with various offset-values.

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Fig. 7 (a) Scattering spectra of the SBGNTs. Scattering spectra of the SBGNT dimers with core offsets perpendicular to the incident polarization for (b) the core offsets at the same sides and (c) the core offsets at the different sides.

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