Efficient low dispersion compact plasmonic-photonic coupler

doi:10.1364/OE.20.012359

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Efficient low dispersion compact plasmonic-photonic coupler

T. P. H. Sidiropoulos, S. A. Maier, and R. F. Oulton »View Author Affiliations

Optics Express, Vol. 20, Issue 11, pp. 12359-12365 (2012)
http://dx.doi.org/10.1364/OE.20.012359

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Abstract

We report efficient low dispersion light coupling into a silicon waveguide using an antenna consisting of two metallic nanoparticles. We find that strong multiple scattering between the nanoparticles dictates the coupling efficiency. We also explore directional coupling, by using different particles with a relative scattering phase, but find that optimum directionality corresponds to minimum efficiency. A dipole model highlights a subtle interplay between multiple scattering and directionality leading to a compromise allowing up to 30% transmission into a single direction. With a 500nm bandwidth near infrared telecoms bands, group delay dispersion is sufficiently low to faithfully couple pulses as short as 50fs.

1. Introduction

The coupling of light into photonic waveguides is a well-known problem, but still topical due to the use of semiconductor materials for compact integrated photonic devices [1

R. G. Hunsperger, Integrated Optics: Theory and Technology (Springer, 2009).

]. Semiconductor waveguides, used in photonics, are smaller than the vacuum wavelength and support high momentum modes that are poorly impedance matched to free space. In principle, prism and grating coupling can overcome these factors [2

H. Raether, Surface Plasmons on Smooth and Rough Surfaces and on Gratings (Springer, 1988).

]; however, prisms are bulky with limited permittivity for coupling to semiconductor waveguides, and the most efficient gratings generally require complicated optimized designs [3

S. Park, G. Lee, S. H. Song, C. H. Oh, and P. S. Kim, “Resonant coupling of surface plasmons to radiation modes by use of dielectric gratings,” Opt. Lett. 28, 1870–1872 (2003). [CrossRef] [PubMed]

]. Simple gratings are typically 20% efficient [4

J. K. Butler, N.-H. Sun, G. A. Evans, L. Pang, and P. Congdon, “Grating-assisted coupling of light between semiconductor and glass waveguides,” J. Lightwave Technol. 16, 1038–1048 (1998). [CrossRef]

]. In addition to a trade-off between design complexity and efficiency, the greatest limitations of these techniques are low bandwidth, high dispersion and high angular sensitivity. Consequently, many researchers and commercial products still use direct end-fire excitation for its simplicity, despite efficiencies as low as just 1% [5

T. D. Happ, M. Kamp, and A. Forchel, “Photonic crystal tapers for ultracompact mode conversion,” Opt. Lett. 26, 1102–1104 (2001). [CrossRef]

–7

V. S. Volkov, Z. Han, M. G. Nielsen, K. Leosson, H. Keshmiri, J. Gosciniak, O. Albrektsen, and S. I. Bozhevolnyi, “Long-range dielectric-loaded surface plasmon polariton waveguides operating at telecommunication wavelengths,” Opt. Lett. 36, 4278–4280 (2011). [CrossRef] [PubMed]

Recent work has looked at reducing the size of grating couplers by using metallic nanoparticles [8

I. P. Radko, S. I. Bozhevolnyi, G. Brucoli, L. Martín-Moreno, F. J. García-Vidal, and A. Boltasseva, “Efficiency of local surface plasmon polariton excitation on ridges,” Phys. Rev. B 78, 115115 (2008). [CrossRef]

–18

J. S. Q. Liu, R. A. Pala, F. Afshinmanesh, W. Cai, and M. L. Brongersma, “A submicron plasmonic dichroic splitter,” Nat. Commun. 2, 525 (2011). [CrossRef] [PubMed]

]. Although the metal’s high permittivity contrast provides stronger scattering [9

A. Ghoshal and P. G. Kik, “Frequency dependent power efficiency of a nanostructured surface plasmon coupler,” Phys. Status Solidi RRL 4, 280–282 (2010). [CrossRef]

], the localized surface plasmon (LSP) resonances [10

V. Giannini, A. I. Fernández-Domínguez, Y. Sonnefraud, T. Roschuk, R. Fernández-García, and S. A. Maier, “Controlling light localization and lightmatter interactions with nanoplasmonics,” Small 6, 2498–2507 (2010). [CrossRef] [PubMed]

] of nanoparticles greatly enhance scattering cross-sections [11

A. Christ, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Waveguide-plasmon polaritons: strong coupling of photonic and electronic resonances in a metallic photonic crystal slab,” Phys. Rev. Lett. 91, 183901 (2003). [CrossRef] [PubMed]

–13

J. K. Day, O. Neumann, N. K. Grady, and N. J. Halas, “Nanostructure-mediated launching and detection of 2D surface plasmons,” ACS Nano 4, 7566–7572 (2010). [CrossRef] [PubMed]

] despite being smaller than the vacuum wavelength [14

S. A. Maier, “Effective mode volume of nanoscale plasmon cavities,” Opt. Quantum Electron. 38, 257–267 (2006). [CrossRef]

]. A number of researchers have exploited this to realize compact couplers using just a few metal nanoparticles [15

T. Kosako, Y. Kadoya, and H. F. Hofmann, “Directional control of light by a nano-optical Yagi-Uda antenna,” Nat. Photon. 4, 312–315 (2010). [CrossRef]

–18

J. S. Q. Liu, R. A. Pala, F. Afshinmanesh, W. Cai, and M. L. Brongersma, “A submicron plasmonic dichroic splitter,” Nat. Commun. 2, 525 (2011). [CrossRef] [PubMed]

]. These works focused primarily on the directional aspect of the coupling without evaluating the potential coupling efficiency.

In this letter, we report an optical antenna that couples a focussed beam into a silicon waveguide mode. Our approach uses the strong light-matter interactions and compactness of plasmonics, while avoiding the high loss associated with plasmonics by radiating rapidly into the photonic mode. Remarkably, we find total coupling efficiencies (into both waveguide directions) of 20% for a single particle and 40% for an identical particle pair at λ ≈ 1.55μm, dropping by only 10% over a broad 400nm range. We find optimal coupling into a single direction of 27% by using two differently shaped particles.

2. Plamsonic-photonic coupling

We investigate two dimensional scattering of light focussed onto gold particles with variable length (L) and thickness (T) embedded in SiO₂ and placed in the vicinity of a photonic Silicon waveguide of thickness (W) (Fig. 1(a)). The particles each support a LSP with dipole moment predominantly along the x̂ direction. An external Gaussian beam, polarized along x̂, excites LSPs, which subsequently re-radiate into the waveguide mode. The coupling rate, κ, between LSPs and waveguide mode is largest when the mode confinement is strongest. There is thus a trade-off between the mode size and the x̂ component of the electric field at the position of the particles. Hence, the coupling rate κ ∝ |E_x(x_NP)|²/ ∫ E(x) × H^*(x)x̂dz. A waveguide thickness of W = 220nm confines the fundamental Transverse Magnetic (TM) mode for optimal coupling near a wavelength of 1.55μm. Meanwhile, the particles are placed as close to the silicon as possible where the mode intensity is greatest (Fig. 1(b)). A 5nm gap avoids direct hybridization of LSPs with the silicon. Finally, the LSP resonances are tuned, by varying the particle length, L, so that the peak in scattering cross section matches the maximum radiative coupling rate of the particle-waveguide system. 20 × 250nm² gold particles embedded in SiO₂ produce a good response (Fig. 1(c)).

Fig. 1 (a) Schematic of the plasmonic antenna. (b) E_x component of the TM waveguide mode at the particle position, normalised to total mode power vs. wavelength. (Insets show the mode’s power profile.) (c) Near field intensity of uncoupled particles for L = 150nm (solid), L = 250nm (dashed; inset shows field distribution 100nm above bulk silicon), and L = 350nm (dotted). (d) Transmission amplitude and phase into one direction of the waveguide for different particle lengths, excited by a 7μm beam, comparing numerically simulation (solid) and a forced dipole model (dotted line).

We first calculate the transmission into the waveguide by a single gold particle. We use a finite element solver (Comsol Multiphysics) in all numerical calculations. We find 4% transmission into the fundamental TM mode at one end of the waveguide from a Gaussian beam focussed to a 7μm diameter spot (Fig. 1(d)). When we add a second particle a distance D from the first, the effective scattering cross section nearly doubles leading to a transmission of just over 7% into one direction, as shown in Fig. 2(a). Here, the de-focussed beam allows us to vary the relative positions of particles with a nearly uniform input field; later, we show how a focused beam significantly increases the transmission.

Fig. 2 Transmission into each direction of the waveguide from two particles excited by a Gaussian beam focussed to a 7μm spot. (a) and (b) show the dependence of transmission on the propagation phase ψ, between two particles for Δ = 0 and Δ = π/4, respectively. The plots compare numerical simulations (open symbols) and the coupled oscillator model with (solid line) and without multiple scattering (dashed line).

3. Coupled dipole oscillator model

The transmission amplitude, t(x), into forward and backward propagating waveguide modes can be modelled by interference of the radiation from two forced coupled dipoles [19

H. A. Haus and W. Huang, “Coupled-mode theory,” Proc. IEEE 79, 1505–1518 (1991). [CrossRef]

t (x) = κ_{1} {\dot{a}}_{1} e^{- i k | x |} + κ_{2} {\dot{a}}_{2} e^{- i k | x - D |} = t_{\pm} e^{\mp i k x},

(1)

where a_i are the dipole amplitudes of the LSPs; and k is the propagation constant of the mode. The left and right transmission coefficients become,

t_{\pm} = s^{- 1} {(\begin{matrix} κ_{1} \\ κ_{2} e^{\pm i ψ} \end{matrix})}^{T} (\begin{matrix} \frac{α_{1}}{κ_{1}} e^{i ϕ_{1}} & - \frac{α_{1} α_{2} β_{1} {\bar{γ}}_{1} e^{i (ϕ_{1} + ϕ_{2} - ψ)}}{κ_{1}} \\ - \frac{α_{1} α_{2} β_{2} {\bar{γ}}_{1} e^{i (ϕ_{1} + ϕ_{2} - ψ)}}{κ_{2}} & \frac{α_{2}}{κ_{2}} e^{i ϕ_{2}} \end{matrix}) (\begin{matrix} c_{1} \\ c_{2} \end{matrix})

(2)

where β_i = κ_i/γ_i are the proportions of light coupled to the waveguide mode; c_i are the coupling coefficients between the input beam and the LSPs and are dependent on the scattering cross-sections of the particles; γ_i are the total LSP extinction rates, including radiation, waveguide coupling and absorption; γ̄_i = γ_i/ω are the total extinction rates normalised to the frequency; α_i = β_i cosϕ_i; ψ = kD; and s = (1 – β₁β₂γ̄₁γ̄₂α₁α₂/4e^{i(ϕ₁+ϕ₂–2ψ)}) describes high order multiple scattering. Note that we have defined the phase of each resonator as

tan ϕ_{i} = (ω_{i}^{2} - ω^{2}) / γ_{i} ω

and therefore cosϕ_i is the amplitude response across the tuning range, |ϕ_i| < π/2.

Following the example of other authors [16

G. Lerosey, D. F. P. Pile, P. Matheu, G. Bartal, and X. Zhang, “Controlling the phase and amplitude of plasmon sources at a subwavelength scale,” Nano Lett. 9, 327–331 (2009). [CrossRef]

, 17

T. Xu, Y. Zhao, D. Gan, C. Wang, C. Du, and X. Luo, “Directional excitation of surface plasmons with subwavelength slits,” Appl. Phys. Lett. 92, 101501 (2008). [CrossRef]

], we examine a simplified solution without multiple scattering by excluding the diagonal terms and setting s = 1, giving the waveguide mode transmission,

T_{\pm} = T_{1} + T_{2} + 2 \sqrt{T_{1} T_{2}} cos (Δ \pm ψ)

(3)

where

T_{i} = c_{i}^{2} α_{i}^{2}

, and Δ = ϕ₂ – ϕ₁. For a single particle the transmission into one direction is T_± = T₁ (Fig. 2(a)). To achieve directional coupling, we must control the relative phase of the two particles by adjusting their length, L.

Figure 1(d) shows the transmission and its phase for a single particle as we detune the LSP at a fixed wavelength of 1.55μm. The transmission and phase approximately follow the expected dependence of the dipole model, T_i(ϕ_i) ≈ T_i(0) cos² ϕ_i. The relative phase between particles can clearly be tuned by more than π/2. (Full 2π phase control can be achieved with more complex 3D nanoparticle geometries [20

N. Yu, P. Genevet, M. A. Kats, F. Aieta, J.-P. Tetienne, F. Capasso, and Z. Gaburro, “Light propagation with phase discontinuities: generalized laws of reflection and refraction,” Science 334, 333–337 (2011). [CrossRef] [PubMed]

].) The transmission curve’s shape, which resembles those in recently reported literature [16

G. Lerosey, D. F. P. Pile, P. Matheu, G. Bartal, and X. Zhang, “Controlling the phase and amplitude of plasmon sources at a subwavelength scale,” Nano Lett. 9, 327–331 (2009). [CrossRef]

, 20

], occurs due to resonance broadening for longer particles. From Eq. (3), the best directional coupling into the forward direction only occurs when both,

\begin{array}{l} ψ + Δ = 2 n π \\ ψ - Δ = (2 m + 1) π \end{array}

(4)

where n,m ∈ 𝕑. However, the total transmission for optimal directionality (Δ = π/2), given by

T = 2 T_{1} + 2 T_{2} + 4 \sqrt{T_{1} T_{2}} cos ψ cos Δ

(5)

is a minimum. For two particles, the total transmission is greatest when T₁ = T₂ and ϕ₂ = ϕ₁ = 0, which also corresponds to least directionality. Furthermore, since T_i ∝ cos²ϕ_i the efficiency for an optimal directional coupler is less than that of an identical particle pair. Directional coupling and optimal efficiency are therefore mutually exclusive. Nevertheless, directional coupling can be effective as shown in Fig. 2(b), where Δ = π/4. Here, a maximum transmission of 11% into one direction can be achieved.

4. Multiple scattering and directional coupling

The asymmetric transmission lineshapes in Figs. 2(a) and 2(b) cannot be explained by the simple interference of two dipoles. A good correspondence between the numerical simulation and Eq. (2) requires strong multiple scattering between the particles. To make the comparison, we have used the analytical transmission trend in Fig. 1(d) with the approximation that β₁ ≈ β₂, γ̄₁ ≈ γ̄₂ and c₁ ≈ c₂, giving only two unknown fitting parameters: the peak transmission of a single particle with zero phase, T₀ = T(ϕ= 0) = 3.5% and the multiple scattering parameter, β²γ̄ ≈ 0.4. The large value of the scattering parameter highlights the strong coupling between nanoparticles and waveguide mode. Furthermore, multiple scattering is sufficiently strong to observe higher order scattering, where s⁻¹ ≈ 1.2. In the absence of multiple scattering, two identical particles should provide four times the single particle transmission, T₀, due to constructive interference, as shown by Eq. (3), for T₁ = T₂ = T₀; ϕ₁ = ϕ₂ = 0. However, with multiple scattering the total transmission for two identical particles is just 4T₀/(1 + β²γ̄)² ≈ 2T₀. Thus, multiple scattering suppresses the constructive interference of the dipoles and reduces the total transmission (Fig. 2(a)). Interestingly, the suppression of interference is less pronounced for Δ = π/4 (Fig. 2(b)).

To further understand the role of multiple scattering, we investigate the two particle coupler’s transmission for various phase differences. To this end, the length of one particle is varied, controlling ϕ₂, while the length of the other is kept constant at L = 250nm, thus fixing the value of ϕ₁ ≈ 0. Figure 3(a) shows the peak transmission for each direction as a function of ϕ₂. While multiple scattering significantly reduces the coupling efficiency for identical particles, the effect is less pronounced for different particles, with a phase difference between them. Hence, when increasing Δ, the transmission also increases approaching the transmission we would expect for constructively interfering particles, near Δ = π/4. It is interesting to note that for Δ > π/4, the transmission surpasses even that of the simple constructively interfering dipoles. Meanwhile, the effect of directional coupling reduces transmission for Δ > π/4, leaving the maximum transmission near Δ ≈ π/4. Multiple scattering is a natural consequence of the extremely strong coupling between nanoparticle and waveguide. For weaker coupling (β²γ̄ ≪ 1) we have observed the constructive interference of each nanoparticle and a total transmission of 4T₀. This suggests that, if β can be maintained at a high value while β²γ̄ ≪ 1, the reduction of multiple scattering could yield even greater coupling efficiencies.

Fig. 3 (a) Maximum transmission (T_max) into left and right directions (open circles and open squares, respectively) vs. phase difference between the two particles for numerical calculations (open symbols) and coupled oscillator model with (solid lines) and without multiple scattering (dashed line). (b) Transmission spectra into one direction for a 2μm focus for two particles with a Δ = π/4 phase shift (solid line; L₁ = 250nm, L₂ = 160nm), an identical particle pair (dotted line; L₁ = L₂ = 250nm), and a single particle (dashed line).

5. Efficient low dispersion coupling

Simply focussing the beam down to a 2μm spot significantly increases the coupling efficiency with the total transmission into one direction reaching 13%, 20% and 27% for the single particle, identical pair and π/4 phase-shifted pair, respectively (Fig. 3(b)). Furthermore, the coupling efficiency is sustained over a bandwidth of at least 500nm. Since scattered light from the plasmonic antenna also only incurs a π phase change across the wide transmission band, we can also expect low group delay dispersion (GDD) of light passing through the coupler, c.f. Fig. 4(a). To calculate pulse broadening we determined the total phase (ϕ) induced by both the coupler and mode propagation over 4μm of the waveguide. The corresponding pulse broadening map is shown in Fig. 4(b). Interestingly, we find anomalous dispersion of our particle coupler that compensates for the normal dispersion on propagating 15μm through the silicon waveguide. With the broad bandwidth and low dispersion, these antennas could faithfully couple the spectral components of pulses as short as 50fs.

Fig. 4 (a) Plasmonic coupler group delay dispersion over transmission window. (b) Pulse broadening due to 4μm propagating along silicon waveguide without coupler (solid), for a particle pair with Δ = π/4 (dashed line), and an identical particle pair (dotted line).

6. Conclusion

In conclusion, we have presented a sub-wavelength optical coupler that is more compact and easier to design than conventional grating couplers yet provides comparable efficiency over a much broader spectrum with low dispersion. Our approach offers directional control through the scattered phase by simply varying each particle’s length. However, coupling efficiency and directionality are mutually exclusive. Meanwhile, multiple scattering between nanoparticles due to the high coupling efficiency suppresses the constructive interference expected of an identical particle pair. Since multiple scattering scales with β²γ̄, we have proposed to reduce it by using resonators with higher Q factors, at the expense of dispersion. To this end, 3D nanoparticles coupled to TM or TE waveguide modes could mitigate multiple scattering. Such waveguide couplers are a viable approach for integrated semiconductor photonics technology due to their ability to achieve high coupling efficiency over a broad wavelength range with extremely low group delay dispersion.

Acknowledgments

This work was sponsored by the UK Engineering and Physical Sciences Research Council (EPSRC). R.F.O. is supported by an EPSRC Fellowship ( EP/I004343/1) and Marie Curie IRG ( PIRG08-GA-2010-277080).

References and links

1.	R. G. Hunsperger, Integrated Optics: Theory and Technology (Springer, 2009).
2.	H. Raether, Surface Plasmons on Smooth and Rough Surfaces and on Gratings (Springer, 1988).
3.	S. Park, G. Lee, S. H. Song, C. H. Oh, and P. S. Kim, “Resonant coupling of surface plasmons to radiation modes by use of dielectric gratings,” Opt. Lett. 28, 1870–1872 (2003). [CrossRef] [PubMed]
4.	J. K. Butler, N.-H. Sun, G. A. Evans, L. Pang, and P. Congdon, “Grating-assisted coupling of light between semiconductor and glass waveguides,” J. Lightwave Technol. 16, 1038–1048 (1998). [CrossRef]
5.	T. D. Happ, M. Kamp, and A. Forchel, “Photonic crystal tapers for ultracompact mode conversion,” Opt. Lett. 26, 1102–1104 (2001). [CrossRef]
6.	C.-W. Liao, Y.-T. Yang, S.-W. Huang, and M.-C. Lee, “Fiber-core-matched three-dimensional adiabatic tapered couplers for integrated photonic devices,” J. Lightwave Technol. 29, 770–774 (2011). [CrossRef]
7.	V. S. Volkov, Z. Han, M. G. Nielsen, K. Leosson, H. Keshmiri, J. Gosciniak, O. Albrektsen, and S. I. Bozhevolnyi, “Long-range dielectric-loaded surface plasmon polariton waveguides operating at telecommunication wavelengths,” Opt. Lett. 36, 4278–4280 (2011). [CrossRef] [PubMed]
8.	I. P. Radko, S. I. Bozhevolnyi, G. Brucoli, L. Martín-Moreno, F. J. García-Vidal, and A. Boltasseva, “Efficiency of local surface plasmon polariton excitation on ridges,” Phys. Rev. B 78, 115115 (2008). [CrossRef]
9.	A. Ghoshal and P. G. Kik, “Frequency dependent power efficiency of a nanostructured surface plasmon coupler,” Phys. Status Solidi RRL 4, 280–282 (2010). [CrossRef]
10.	V. Giannini, A. I. Fernández-Domínguez, Y. Sonnefraud, T. Roschuk, R. Fernández-García, and S. A. Maier, “Controlling light localization and lightmatter interactions with nanoplasmonics,” Small 6, 2498–2507 (2010). [CrossRef] [PubMed]
11.	A. Christ, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Waveguide-plasmon polaritons: strong coupling of photonic and electronic resonances in a metallic photonic crystal slab,” Phys. Rev. Lett. 91, 183901 (2003). [CrossRef] [PubMed]
12.	J.-P. Tetienne, A. Bousseksou, D. Costantini, Y. De Wilde, and R. Colombelli, “Design of an integrated coupler for the electrical generation of surface plasmon polaritons,” Opt. Express 19, 18155–18163 (2011). [CrossRef] [PubMed]
13.	J. K. Day, O. Neumann, N. K. Grady, and N. J. Halas, “Nanostructure-mediated launching and detection of 2D surface plasmons,” ACS Nano 4, 7566–7572 (2010). [CrossRef] [PubMed]
14.	S. A. Maier, “Effective mode volume of nanoscale plasmon cavities,” Opt. Quantum Electron. 38, 257–267 (2006). [CrossRef]
15.	T. Kosako, Y. Kadoya, and H. F. Hofmann, “Directional control of light by a nano-optical Yagi-Uda antenna,” Nat. Photon. 4, 312–315 (2010). [CrossRef]
16.	G. Lerosey, D. F. P. Pile, P. Matheu, G. Bartal, and X. Zhang, “Controlling the phase and amplitude of plasmon sources at a subwavelength scale,” Nano Lett. 9, 327–331 (2009). [CrossRef]
17.	T. Xu, Y. Zhao, D. Gan, C. Wang, C. Du, and X. Luo, “Directional excitation of surface plasmons with subwavelength slits,” Appl. Phys. Lett. 92, 101501 (2008). [CrossRef]
18.	J. S. Q. Liu, R. A. Pala, F. Afshinmanesh, W. Cai, and M. L. Brongersma, “A submicron plasmonic dichroic splitter,” Nat. Commun. 2, 525 (2011). [CrossRef] [PubMed]
19.	H. A. Haus and W. Huang, “Coupled-mode theory,” Proc. IEEE 79, 1505–1518 (1991). [CrossRef]
20.	N. Yu, P. Genevet, M. A. Kats, F. Aieta, J.-P. Tetienne, F. Capasso, and Z. Gaburro, “Light propagation with phase discontinuities: generalized laws of reflection and refraction,” Science 334, 333–337 (2011). [CrossRef] [PubMed]

OCIS Codes
(130.4310) Integrated optics : Nonlinear
(230.7380) Optical devices : Waveguides, channeled
(230.4555) Optical devices : Coupled resonators
(250.5403) Optoelectronics : Plasmonics

ToC Category:
Optics at Surfaces

History
Original Manuscript: February 22, 2012
Revised Manuscript: March 27, 2012
Manuscript Accepted: March 27, 2012
Published: May 16, 2012

Citation
T. P. H. Sidiropoulos, S. A. Maier, and R. F. Oulton, "Efficient low dispersion compact plasmonic-photonic coupler," Opt. Express 20, 12359-12365 (2012)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-20-11-12359

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References

R. G. Hunsperger, Integrated Optics: Theory and Technology (Springer, 2009).
H. Raether, Surface Plasmons on Smooth and Rough Surfaces and on Gratings (Springer, 1988).
S. Park, G. Lee, S. H. Song, C. H. Oh, and P. S. Kim, “Resonant coupling of surface plasmons to radiation modes by use of dielectric gratings,” Opt. Lett.28, 1870–1872 (2003). [CrossRef] [PubMed]
J. K. Butler, N.-H. Sun, G. A. Evans, L. Pang, and P. Congdon, “Grating-assisted coupling of light between semiconductor and glass waveguides,” J. Lightwave Technol.16, 1038–1048 (1998). [CrossRef]
T. D. Happ, M. Kamp, and A. Forchel, “Photonic crystal tapers for ultracompact mode conversion,” Opt. Lett.26, 1102–1104 (2001). [CrossRef]
C.-W. Liao, Y.-T. Yang, S.-W. Huang, and M.-C. Lee, “Fiber-core-matched three-dimensional adiabatic tapered couplers for integrated photonic devices,” J. Lightwave Technol.29, 770–774 (2011). [CrossRef]
V. S. Volkov, Z. Han, M. G. Nielsen, K. Leosson, H. Keshmiri, J. Gosciniak, O. Albrektsen, and S. I. Bozhevolnyi, “Long-range dielectric-loaded surface plasmon polariton waveguides operating at telecommunication wavelengths,” Opt. Lett.36, 4278–4280 (2011). [CrossRef] [PubMed]
I. P. Radko, S. I. Bozhevolnyi, G. Brucoli, L. Martín-Moreno, F. J. García-Vidal, and A. Boltasseva, “Efficiency of local surface plasmon polariton excitation on ridges,” Phys. Rev. B78, 115115 (2008). [CrossRef]
A. Ghoshal and P. G. Kik, “Frequency dependent power efficiency of a nanostructured surface plasmon coupler,” Phys. Status Solidi RRL4, 280–282 (2010). [CrossRef]
V. Giannini, A. I. Fernández-Domínguez, Y. Sonnefraud, T. Roschuk, R. Fernández-García, and S. A. Maier, “Controlling light localization and lightmatter interactions with nanoplasmonics,” Small6, 2498–2507 (2010). [CrossRef] [PubMed]
A. Christ, S. G. Tikhodeev, N. A. Gippius, J. Kuhl, and H. Giessen, “Waveguide-plasmon polaritons: strong coupling of photonic and electronic resonances in a metallic photonic crystal slab,” Phys. Rev. Lett.91, 183901 (2003). [CrossRef] [PubMed]
J.-P. Tetienne, A. Bousseksou, D. Costantini, Y. De Wilde, and R. Colombelli, “Design of an integrated coupler for the electrical generation of surface plasmon polaritons,” Opt. Express19, 18155–18163 (2011). [CrossRef] [PubMed]
J. K. Day, O. Neumann, N. K. Grady, and N. J. Halas, “Nanostructure-mediated launching and detection of 2D surface plasmons,” ACS Nano4, 7566–7572 (2010). [CrossRef] [PubMed]
S. A. Maier, “Effective mode volume of nanoscale plasmon cavities,” Opt. Quantum Electron.38, 257–267 (2006). [CrossRef]
T. Kosako, Y. Kadoya, and H. F. Hofmann, “Directional control of light by a nano-optical Yagi-Uda antenna,” Nat. Photon.4, 312–315 (2010). [CrossRef]
G. Lerosey, D. F. P. Pile, P. Matheu, G. Bartal, and X. Zhang, “Controlling the phase and amplitude of plasmon sources at a subwavelength scale,” Nano Lett.9, 327–331 (2009). [CrossRef]
T. Xu, Y. Zhao, D. Gan, C. Wang, C. Du, and X. Luo, “Directional excitation of surface plasmons with subwavelength slits,” Appl. Phys. Lett.92, 101501 (2008). [CrossRef]
J. S. Q. Liu, R. A. Pala, F. Afshinmanesh, W. Cai, and M. L. Brongersma, “A submicron plasmonic dichroic splitter,” Nat. Commun.2, 525 (2011). [CrossRef] [PubMed]
H. A. Haus and W. Huang, “Coupled-mode theory,” Proc. IEEE79, 1505–1518 (1991). [CrossRef]
N. Yu, P. Genevet, M. A. Kats, F. Aieta, J.-P. Tetienne, F. Capasso, and Z. Gaburro, “Light propagation with phase discontinuities: generalized laws of reflection and refraction,” Science334, 333–337 (2011). [CrossRef] [PubMed]

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