Plasmonic bandgap in random media
© Zhurikhina et al.; licensee Springer. 2013
Received: 6 June 2013
Accepted: 9 July 2013
Published: 16 July 2013
We present a dispersion theory of the surface plasmon polaritons (SPP) in random metal-dielectric nanocomposite (MDN) consisting of bulk metal embedded with dielectric inclusions. We demonstrate that embedding of dielectric nanoparticles in metal results in the formation of the plasmonic bandgap due to strong coupling of the SPP at the metal-vacuum interface and surface plasmons localized at the surface of nanoinclusions. Our results show that MDN can replace metals in various plasmonic devices, which properties can be tuned in a wide spectral range. Being compatible with waveguides and other photonic structures, MDN offers high flexibility in the plasmonic system design.
78.67.Sc, 81.05.Ni, 71.36.+c
The resonant coupling of light to oscillations of the free electron density near the metal surface, surface plasmons (SP), gave birth to a variety of advanced applications ranging from sensing to nonlinear optics. SPs are bound to the metallic surface, i.e., at the frequency of the surface plasmon resonance, light field exponentially decays in neighboring media. Since the decay length of SPs is two orders of magnitude smaller than the wavelength of the light in air, they can be employed for subwavelength localization of light. The guiding of light in plasmonic structures is possible via surface plasmon polaritons (SPP) that can propagate in periodical arrays of metal nanoparticles embedded in dielectrics. The multiple scattering of the SPPs off the periodic corrugation leads to the Bragg-like plasmon modes [1, 2] and to the plasmonic band gaps [1, 3], i.e., they do not allow the SPP in a certain interval of wavelengths. When metal nanoparticles are placed into dielectric in a random fashion, e.g., in metal island films [4, 5], nanoporous metal films , and metal-dielectric nanocomposite (MDN) [7–10], no SPP bandgaps have been observed. The optical properties of these materials dominated by SPs localized on individual metal nanoparticles are well studied [11, 12]; however, much less attention was paid to the behavior of SPP propagating at the MDN-dielectric interface. In this paper, we present the theory of SPP in MDN based on noble metals with random distribution of the dielectric inclusions. We demonstrate that when the metal volume content is high, the coupling of propagating and localized at metal-inclusion interface plasmon modes results in the formation of the SPP bandgap in such random media. By using Drude model for dielectric function of the metal, we develop dispersion theory of the SPP at the MDN-vacuum surface. We demonstrate that in silver, bandgap persists when dielectric properties of the metal are described by experimental data. The presence of the SPP bandgap indicates that the MDN can replace metals in various plasmonic structures that will benefit from the tunability of the MDN properties.
One can observe from Equations 1 and 2 that SPP is allowed at Re(ϵ2(ω) + ϵ1) < 0 when Re(k SPP ) ≠ 0 and Im(δ1,2) = 0. The condition Re(ϵ2(ω) + ϵ1) = 0 corresponds to the excitation of the surface plasmon [1, 13]. If Re(ϵ2(ω)) > 0, SPP is forbidden; however, a transversal bulk plasmon polariton (BPP) with wave vector can propagate at z > 0. If 0 > Re(ϵ2(ω)) > − ϵ1, no propagating electromagnetic perturbations are allowed, i.e., the energy of the incident light wave is transferred to the localized plasmons.
One can see from Equation 5 that the effective dielectric function has singularities at ω = 0 and ω = ΩTO. The singularity at ω = 0 is a conventional ‘metal’ one, while the singularity at ω = ΩTO corresponds to the collective oscillations of the conduction electrons at the surface of dielectric nanoparticles incorporated into the metal matrix, i.e., localized surface plasmon resonance at the metal-dielectric interface. Frequency ΩLO corresponds to the excitation of the longitudinal phonons in the GMN.
Results and discussion
The dispersion relation for propagating electromagnetic modes in Drude MDN with dielectric volume fraction g = 0.1 and ϵd = 3.42 is shown in Figure 1a. Figure 1b shows the map of collective excitations in Drude MDN in the ‘ω-g’ plane at ϵd= 3.42. One can observe two SPP bands, the BPP band, and the forbidden gap separated by frequencies ΩLO, ΩTO, and ωSC1. The upper limit of the higher SPP zone is ωSC2. There also exists the second BPP frequency range for ω > ωp. The width of both SPP and BPP bands increases with the increase of dielectric contained in MDN. The latter was earlier demonstrated by N. Stefanou and coauthors  for mesoporous metals. Our calculations also showed that the higher the permittivity of dielectric inclusions in MDN, the broader the upper SPP band and the bigger the downshift of the SPP forbidden gap.
When g → 0, the upper MDN surface plasmon frequency , that is, the surface plasmon frequency at metal-air interface, while ΩLO, ΩTO, and ωSC1 approach , that is, the SP resonance of a single dielectric cavity in metal matrix . At ϵd > 2, the frequencies ΩLO, ΩTO, and ωSC1 are lower than ωSC2, and BPP zone and the conventional metal SPP band at ω < ωSC2 splits by two (see Figure 1b). At ϵd < 2, the ΩLO, ΩTO, and ωSC1 are higher than ωSC2, and the conventional metal SPP band at ω < ωSC2 remains intact, however, the second SPP band appears at ωLO< ω < ωSC2. At .
It is worth noting that the dielectric dispersion should change the characteristic frequencies that will lead to the frequency shift of all bands and, in the case of strong dispersion, could possibly result in broadening or vanishing of the second SPP band. But for the most optically transparent dielectrics, their dispersion is negligible compared to the metal one. In this paper we neglect the dielectric dispersion that is valid, for example, for glasses in the visible and near-infrared range.
Figure 3b shows the map of collective excitations in silver-based MDN on the ω-g plane at ϵd = 3.42. One can observe that the shape and size of the gray area in which SPP is allowed is similar to that for Drude MDN (see Figure 1); however, the nonzero imaginary part of the dielectric permittivity of silver results in vanishing of the SPP bandgap at g < 0.03. Thus, only one surface plasmon polariton band exists at g < 0.03.
We demonstrate that SPP bandgap can exist not only in plasmonic crystals but also in MDN with low dielectric volume fraction, i.e., when dielectric nanoinclusions are distributed in a random fashion in metal host. In the MDN, the SPP bandgap arises due to strong coupling between SPP at the metal-dielectric interface and plasmons localized on dielectric nanoinclusions allowing one to tailor the plasmonic properties by changing the dielectric content. By using Maxwell-Garnett model, we calculated effective dielectric permittivity of the MDN using both Drude model and Johnson and Christy data for complex dielectric function of metal. We showed that dissipation caused by the scattering of conduction electrons in metal may result in vanishing plasmonic bandgap in noble metal-based MDN. However, at refractive index of dielectric inclusions n > 1.5, the plasmonic bandgap survives in Ag-based MDN offering high flexibility in the plasmonic system design.
VZh holds associate professor position at St. Petersburg State Polytechnical University. MP holds PhD degree at St. Petersburg Academic University. OSh is a PhD student at St. Petersburg State Polytechnical University. YuS holds DrSci degree and professor position at the University of Eastern Finland. AL holds DrSci degree and professor positions at St. Petersburg Academic University and St. Petersburg State Polytechnical University.
Surface plasmon polaritons.
This study was supported by Russian foundation for Basic Research (project no. 12-02-91664), Russian Ministry for Education and Science, Joensuu University Foundation, Academy of Finland (project nos. 135815 and 137859) and EU (FP7 projects ‘NANOCOM’ and ‘AN2’).
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