3D conductive coupling for efficient generation of prominent Fano resonances in metamaterials

Abstract

We demonstrate a 3D conductive coupling mechanism for the efficient generation of prominent and robust Fano resonances in 3D metamaterials (MMs) formed by integrating vertical U-shape split-ring resonators (SRRs) or vertical rectangular plates along a planar metallic hole array with extraordinary optical transmission (EOT). In such a configuration, intensified vertical E-field is induced along the metallic holes and naturally excites the electric resonances of the vertical structures, which form non-radiative "dark" modes. These 3D conductive "dark" modes strongly interfere with the "bright" resonance mode of the EOT structure, generating significant Fano resonances with both prominent destructive and constructive interferences. The demonstrated 3D conductive coupling mechanism is highly universal in that both 3D MMs with vertical SRRs and vertical plates exhibit the same prominent Fano resonances despite their dramatic structural difference, which is conceptually different from conventional capacitive and inductive coupling mechanisms that degraded drastically upon small structural deviations.

R

A P

,* ,* ,

Plasmonic Fano resonances in nanostructures and metamaterials (MMs) have attracted great attention due to their promising applications in ultrasensitive biosensing, high-contrast optical imaging, high-quality optical waveguides, as well as new types of nonlinear and switchable metamaterials14. As a result, the efficient generation of plasmonic Fano resonances has raised extensive interest in recent years, and a wide variety of approaches and geometries have been proposed and explored, such as nanoparticle clusters5,6, nonconcentric nanoparticles7,8, composite split-ring resonators (SRR)4,9,10, perforated metallic lms11, metallic photonic crystals12, etc. Generally, two schemes could be utilized for the generation of Fano resonances. The rst type of plasmonic Fano resonance could be induced by the coherent interference between spectrally-overlapped superradiant dipole modes and subradiant high-order modes, i.e. by the coupling between broad bright modes and narrow dark modes8,13,14. For

example, in non-concentric ring/disk cavity systems, the broad dipole modes of the disks were interfered with the narrow high-order modes (dark modes) of the rings, resulting in Fano resonance with strong sensitivity to the environments8,10. As the second type, the plasmonic hybridization between spectrally-overlapped dipole modes (both are bright modes) of adjacent nanoparticles could also generate versatile Fano resonances, which has been widely employed in the so-called plasmonic oligomers (or nanoparticle clusters)1517. So far, most plasmonic Fano resonances were reported in two-dimensional (2D) systems and more or less encountered constraints: in the former case, the high-order dark resonance modes were normally weak and not easily accessible3, for the latter type, the plasmonic hybridizations were extremely sensitive to the plasmonic gaps between neighboring nanoparticles, which are difficult for controllable fabrications15,18.

The coupling mechanisms available for the plasmonic Fano resonances could be summarized into three types, i.e. capacitive (electric) coupling, inductive (magnetic) coupling and conductive (connective) coupling1820.

Among them, the capacitive coupling depends on the charge oscillations on the two sides of the plasmonic gaps15,21 and the inductive coupling relies on the current ows in coil-type congurations10,20,22, both of which are well known and have been widely adopted in the generation of plasmonic Fano resonance13. In comparison, the conductive coupling has been largely overlooked due to its simple conguration at the rst sight (i.e. the 2D conductive structures look like simple electric connection of individual elements), although it has exhibited strong impacts on the modications of plasmonic properties in systems such as gold nanorod dimers23,24, theta-shaped

Collaborative Innovation Center of *

SCIENTIFIC REPORTS

1

www.nature.com/scientificreports/

Figure 1. Prominent Fano resonances in 3D MMs. (a) Schematic of the unit cell of a 3D MM in which the vertical SRR or vertical plate (SRR lled with the grey area) is conductively connected to one edge of a metallic hole. The free-standing structure is completely composed of Au without any substrate. (b,c) Side-view SEM images of the fabricated 3D MMs with (a) vertical SRRs and (b) vertical plates, respectively. Scale bars: 500nm.(d) As-measured and (e) calculated transmission spectra of an EOT structure without any vertical structure and two 3D MMs with dierent vertical structures under y-polarized light excitation. The Fano resonances of the two 3D MMs are well preserved under the dramatic structural changes. Structural parameters: p=750nm, a=560nm, d=50nm; l=430nm, h=560nm, w= 150nm; width and height of the vertical plates: lp=430nm, hp=560nm. (f) Measured and calculated transmission spectra of a 3D MM under y-polarized light excitation in the mid-infrared wavelength region, agreeing very well with each other. Structural parameters: p=3m, a=2m, d=80nm, l=1m, h=1.45m, w=0.25m.

ring-rod nanostructures19, and THz connected SRR structures18. The main reason is that the 2D connected elements were generally treated as single conductive structures and the resulted couplings were traditionally rationalized as the interference between the bright dipole modes and the dark high-order modes19.

Recently we observed signicant Fano resonances from a nanograter-like 3D MM formed by integrating vertical U-shape SRRs along a planar metallic hole array and explained the observations phenomenologically and qualitatively by traditional plasmonic hybridizations25. In this work we demonstrate an even simpler 3D MMs with micro-plates to generate signicant Fano resonance without the use of SRR-type building blocks. It is found that a 3D conductive coupling mechanism is the actual physical mechanism for the efficient generation of prominent Fano resonances in both 3D MMs. In this mechanism, when the metallic hole array with extraordinary optical transmission (EOT) is illuminated by normal incident light, the excited surface plasmon polaritons (SPPs) with electric-eld (E-eld) polarized perpendicular to the 2D array plane can efficiently activate vertical electric currents in the vertical nanostructures (vertical SRRs or vertical micro-plates), which naturally introduce dark modes. This 3D conductive dark mode strongly interferes with the bright dipole-like resonance mode of the EOT structure, which forms pronounced Fano resonances with both prominent destructive and constructive interferences. We show that once the conditions for this mechanism are satised, the prominent Fano resonances could be well preserved no matter the vertical structures are SRRs or micro-plates. Therefore, our 3D conductive coupling induced prominent Fano resonances are very robust and conceptually dierent from conventional capacitive and inductive coupling schemes that degrade drastically upon small structural deviations.

Figure1a illustrates the schematic of the 3D MMs in our studies, which are formed by vertical U-shape SRRs or vertical rectangular micro-plates standing along a planar metallic hole array. The U-shape SRRs have been the popular and widely accepted building blocks for various 2D and 3D MMs in which the electric resonances could be excited by E-eld parallel to the two arms (Ez) and the magnetic resonances can be excited by E-eld perpendicular to the two arms while parallel to the U-plane (Ex)26. It should be mentioned that in most cases, the SRR-based MMs employed isolated SRRs with planar27, vertical28,29 or multi-layer arrangements30, which mainly relied on electric coupling, magnetic coupling or their combinations. In comparisons, the congurations like in Fig.1a are not traditionally considered due to the lack of knowledge in conductive coupling, as well as the difficulties in fabrications of such 3D nanostructures.

SCIENTIFIC REPORTS

2

www.nature.com/scientificreports/

By using an in situ focused-ion-beam (FIB) irradiation-induced folding technique that we recently developed (see Methods)25, it is very sophisticated to realize such kinds of 3D MMs in free-standing Au lms, as shown in Fig.1b (a 3D MM with vertical SRRs) and Fig.1c (a 3D MM with vertical plates), respectively. Surprisingly, the transmission spectra of both 3D MMs exhibit signicant Fano-like resonances in both long wavelength and short wavelength regions (named as Fano resonance #1 and #2, respectively) as plotted in Fig.1d, forming sharp contrast to the spectrum of the EOT structure without any vertical structures (grey line in Fig.1d). This preservation of Fano resonances upon drastic structural changes is well veried by our numerical simulations in Fig.1e, indicating that the central gap of the vertical SRRs does little eects to the generation of prominent Fano resonances. These ndings are very important from two aspects. Firstly, compared to the 3D MMs with SRRs, the 3D MMs with micro-plates have obvious advantages on fabrication efficiency (33% reduction in fabrication time) due to their simpler geometry and mechanical stabilities due to the less overhanging structures. Secondly, these observations indicate an underlying physical mechanism responsible for the generation of prominent Fano resonances, which might be universal for the designs of other types of 3D MMs with versatile Fano resonances and thus deserves in-depth studies.

One may notice that except the emerging of both Fano resonances in similar wavelength regions with the same trend, some details of the measured and calculated results in Fig.1d,e are not well matched. In comparison, the measured transmission spectrum of a 3D MM with SRRs in mid-infrared wavelength region, as plotted in Fig.1f, is nearly perfectly matched with the calculation. This could be caused by the fact that in the realistic cases, the structures with tiny features normally suer from relative larger fabrication imperfections than structures with larger sizes. Meanwhile, the material constants employed in modellings may deviate from realistic materials more seriously in high-frequency region than those in low-frequency region. Therefore, to eectively nd out the underlying physical mechanism responsible for the Fano resonances, we move the studies to mid-infrared wavelength region, where experimental observations and numerical simulations are more consistent (Fig.1f) and the principles can be generally applied.

On the other hand, since reported in 1998 by Ebbesen and co-workers31, the EOT in a metallic hole array has been well recognized as the result from two resonances, i.e. the surface plasmon resonances (SPRs) due to the periodicity and the localized plasmonic waveguide modes within the holes32,33. Importantly, the SPRs of the EOT structure could induce signicantly enhanced E-eld along the metallic holes in the z direction (Ez) when excited by y-polarized light, as plotted in Fig.2a. Therefore, when a vertical SRR or vertical plate is placed within the intensied Ez eld (as the dashed outlines in Fig.2a), the electric resonances of the vertical structure could be naturally and efficiently excited. The corresponding excitation efficiency will be the highest if the vertical structure is electrically connected to the edge of the metallic hole due to the fact that the intensied Ez eld is strongest at the air/metal interface. As a result, Fig.2be plot two resonant electric current ows along the vertical SRRs and vertical plates of the 3D MMs, respectively. It can be seen that Mode #1 represents an in-phase conductive current ow while Mode #2 denotes an anti-phase current ow. Due to symmetry constraints, only currents that are parallel to the incident E-eld can radiate into the far eld18. Therefore, under y-polarized incident E-eld, both modes (Modes #1 and #2) associated with vertical (z-direction) currents ows are non-radiative and naturally dark modes. These 3D conductive connection induced dark modes could strongly couple with the dipole-like SPR resonance of the EOT structure (the whole process is called as 3D conductive coupling), which nally results in prominent Fano-like resonances. As plotted in Fig.2f, the sharp and asymmetric spectral proles of the Fano resonance (red and black lines) in the 3D conductive MMs exhibit dramatic dierences to that of the EOT structure (grey line). More importantly, it can be seen that the transmission spectra from the 3D MMs with vertical SRRs (red line) and vertical plates (black line) are almost the same, mainly caused by the fact that the 3D conductive coupling processes in both structures are mostly similar, as illustrated in Fig.2b,e.

To further demonstrate the importance of the 3D conductive coupling mechanism, the vertical SRRs are intentionally lied from the in-plane EOT structure in Fig.2g, in the case of which capacitive coupling could be initiated when the gap distance (g) is larger than zero. It can be seen from Fig.2f that when the gap distance is increased to 100 nm (corresponding to ~/45), i.e. when the condition changes from conductive coupling to capacitive coupling, the peak-to-dip depth of Fano resonance #1 degrades dramatically (blue curve). This observation clearly proves that the 3D conductive coupling mechanism plays a major role in the generation of prominent Fano resonance #1. It should be emphasized that the 3D conductive coupling induced Fano resonances only exist under y-polarized excitation. When excited by x-polarized incident light, as shown in Fig.2h, the transmission of the 3D MMs with dierent gap distance shows little spectral shi. In this case, the spectra of the 3D MMs simply represent the linear spectral overlapping between the SRR and EOT structures, indicating there is almost no couplings between the SRR and EOT structures when g> 50nm although the magnetic resonance of the SRR (plotted by the triangles in Fig.2h) could be separately excited by x-polarized light. It should be mentioned that the tiny spectral dip at 4m in the case of g= 0 results from the modied magnetic resonance of the SRR when it is connected to the EOT structure.

For quantitative comparisons, in Fig.3a we normalize the transmission spectra of the 3D MM to that of the EOT structure under y-polarized excitation when the coupling scheme varies gradually from 3D conductive coupling (g= 0nm) towards capacitive coupling (g> 0nm). One can clearly see that for g= 0nm and near Fano resonance #1, signicant constructive (enhanced by ~52% at the peak) and destructive (suppressed by ~92% at the dip) interference eects are observed in the case of y-polarized excitation. This is quite consistent with the classical understanding that Fano resonance describes both destructive and constructive interferences between a discrete state and a continuum state2. Meanwhile, it is found that for Fano resonance #1, both the resonance wavelength and the amplitude of constructive and destructive interferences are highly sensitive to the gap distance. Its peak-to-dip depth drops quickly by 75% when the 3D MM deviates slightly from conductive coupling (g=0nm) to capacitive coupling with a gap distance as small as /20 (g= 150nm), as shown in Fig.3b, further illustrating

SCIENTIFIC REPORTS

3

www.nature.com/scientificreports/

Figure 2. Modellings and simulations. (a) Simulated E-eld distribution (indicated by dark arrows) of an EOT structure (a pure metallic hole array without SRRs) in the yz plane. Ez is plotted in color. The solid red lines outline the structural prole and the dashed red lines indicate the position of the vertical structure where Ez is naturally intensied and can efficiently drive the electric current ow in the vertical structure. (Inset) Dipole-like E-eld distribution of EOT structure in xy plane. (be) Simulated current distributions of the 3D MMs with (b,c) vertical SRRs and (d,e) vertical plates, respectively, at two distinct modes (named as #1 and #2). As noted by the arrows, Mode #1 represents an in-phase conductive current ow while Mode #2 denotes an anti-phase current ow. The similarities between (b,d), as well as (c,e), indicate the same underlying physical mechanism. (f) Simulated transmission spectra of an EOT structure, a 3D MM with vertical plates, a 3D MM with vertical SRRs and a 3D MM with lied vertical SRRs with a gap distance of g under y-polarized light excitation. The arrow indicates the periodicity of the structural lattice. (g) Schematic of the unit cell of a 3D MM in which the vertical SRR is lied above the EOT structure by a gap distance of g. (h) Simulated transmission spectra of an EOT structure, an SRR array, and 3D MMs with dierent g (unit: nm) under x-polarized excitation. Structural parameters: p=3m, a=2m, d=80nm, l=0.9m, h=0.8m, w=0.25m; width and height of the vertical plates: lp=0.9m, hp=0.8m.

the critical role of the 3D conductive coupling. In comparison, both resonance wavelength and amplitude of Fano resonance #2 change more slowly with the gap distance. This is because for the anti-phase coupling case of Mode #2, the repelling currents in SRR and EOT structure are relatively independent even when the two structures are electrically conducted. Therefore, the 3D conductive coupling eect in Fano resonance #2 is much weaker than that in Fano resonance #1.

From above analysis, it is now clear that the prerequisites for 3D conductive coupling include two parts: the rst part is a planar structure that couples efficiently with incident light and supports SPR-enhanced vertical E-eld (Ez); the second part is a vertical structure that can sustain vertical electric resonances within the intensied Ez eld. As long as these two prerequisites are satised, prominent Fano resonances could be generated without the need of complicated formulas, models, or mechanisms34. Therefore, since the electric current ows are mostly along the outer edges of the SRRs under y-polarized excitation (Fig.2b,c), simply replacing the SRR

SCIENTIFIC REPORTS

4

www.nature.com/scientificreports/

Figure 3. Comparisons between 3D conductive coupling and capacitive coupling. (a) Normalized transmission spectra of the 3D MMs with SRRs to that of EOT structure under dierent gap distances (unit: nm) upon y-polarized excitation. (b) (le) Absolute peak-to-dip depth and (right) dip wavelength as a function of the gap distance for resonances #1 and #2, respectively. Structural parameters are the same as in Fig.2 except the gap distance g. Fano resonance #1 is mainly resulted from the 3D conductive coupling, which will be more discussed in following studies.

structure with a vertical rectangular plate of the same size does not change the two prerequisites for prominent Fano resonances (Fig.2d). Consequently, the 3D MMs with vertical SRRs and vertical plates possess signicant Fano resonances at nearly the same spectral positions, as shown in Fig.1df, verifying the robust and universal generation of Fano resonances with the 3D conductive coupling mechanism. One may notice that the position and depth of the measured Fano resonance #1 in Fig.1d are nearly unchanged while its width is broadened due to the less connement of the electric charges, which induces extra non-radiative losses. Nevertheless, this preservation of Fano resonances when deviating dramatically from vertical SRRs to vertical plates clearly proves the robustness upon fabrications, which are highly desirable for large-scale or stream-lined fabrications. In other words, the introduction of Fano resonances in our 3D MMs is simply dependent on the eective conductive coupling length. Therefore, by engineering the 3D conductive coupling length through varying the size of the metallic holes, the width and height of the vertical structures, the Fano resonances in 3D MMs could be widely tuned from near-infrared to mid-infrared wavelength region, as illustrated in Fig.1d,f, which are very preferable for applications in tunable MMs.

Another important feature of the proposed 3D conductive coupling is that the induced Fano resonance #1 exhibits characteristics of localized resonance. As the simulation results shown in Fig.4a, the position of Fano resonance is well preserved under normal incidence, irrespective of the polarization angles (except that both Fano resonances disappear under x-polarized excitation). The suppression factor at the Fano resonance (#1) dip versus the in-plane polarization angle exhibits a strong dipole-like pattern in the polar plot (as shown in Fig.4b), indicating the strongly localized and anisotropic features of the Fano resonance. Interestingly, there is a crossing point near Fano resonance #1 where the transmission is xed for all polarization angles (as indicated by the red arrow Fig.4a), which is highly preferable for polarization-insensitive optical sensing. These features, including the crossing point, are well veried by our experimental results in Fig.4c. Moreover, measurements under y-polarized excitation (Fig.4d) also show that the position of Fano resonance #1 is almost independent on the illumination angle under y-polarized excitation, while Fano resonance #2 that is less aected by the 3D conductive coupling changes dramatically. This robustness of Fano resonance #1 (with wavelength variation of less than 2% for both simulations and measurements in Fig.4ad) results from the facts that except the excitation efficiency, the dierent illumination schemes in Fig.4ad do not change the basic conditions for the generation of Fano resonances, i.e. the E-eld of the planar SPPs is intrinsically along the vertical direction and the SRRs are vertically connected with the planar structures. Therefore, it could be concluded that the 3D conductive coupling induced Fano resonance #1 is a type of localized resonance and thus its position is polarization-insensitive. These interesting polarization properties of the 3D conductive coupling induced Fano resonances may provide new prospects for the emerging areas of meta-surfaces35,36.

In summary, we have demonstrated a 3D conductive coupling mechanism for the efficient generation of robust and prominent Fano resonances in a new type of 3D MMs. Based on the 3D conductive coupling mechanism, only two simple prerequisites are required for the generation of Fano resonances, i.e. a planar structure providing intensied vertical E-eld on the surface (like EOT structure) and a vertical structure sustaining electric resonances (like vertical SRRs or vertical plates). In such a conguration, electric dark modes could be naturally induced and strongly interfere with the bright dipole-like resonance mode of the EOT structure. As a result, we have observed pronounced Fano resonances with both prominent destructive and constructive interferences in both simulations and experiments. Moreover, we have shown that the 3D conductive coupling mechanism is highly universal in that both 3D MMs with vertical SRRs and vertical plates exhibited the same prominent Fano resonances although their structural geometries were largely dierent. Last but not least, the 3D conductive coupling induced Fano resonance exhibits characteristics of localized resonance, of which the

SCIENTIFIC REPORTS

5

www.nature.com/scientificreports/

Figure 4. Prominent Fano resonances with polarization-independent spectral position. (a) Calculatedand (c) measured transmission spectra of a 3D MM under normal incidence with dierent polarization angle as illustrated in the inset. = 90 means y-polarized excitation. The small peaks at approximately 4.2 m are caused by the unstable absorption from CO2 in the FTIR chamber. (b) Polar plot of the calculated suppression factor (dened as the dierence in transmission between the 3D MM and EOT structure divided by the transmission of the EOT structure) at the dip wavelength of Fano resonance #1 as a function of the polarization angle under normal incidence. (d) Measured transmission spectra of the 3D MM under y-polarized excitation with dierent incident angle as illustrated in the inset. Structural parameters are the same as in Fig.1f. The variations of dip wavelength of Fano resonance #1 in (ad) are less than 2%, while the resonance strengths are changed due to the dierent excitation efficiency of SPPs under varied illumination schemes.

wavelength position is immune against certain changes in illumination polarizations. Therefore, our 3D conductive coupling mechanism is simple, universal, robust, and conceptually dierent from conventional capacitive and inductive coupling mechanisms that degraded drastically upon small structural deviations. This work could provide a new methodology for the efficient generation of Fano resonances with simple geometries, fast fabrications, stable mechanical strength, etc., holding potential applications in enhanced extraordinary optical transmission, color displays, optical sensing, etc., as well as opening up new prospects for the emerging areas of metasurfaces35,36.

The 3D MMs were fabricated with a focused-ion-beam (FIB) irradiation-induced folding technique on self-supporting Au lms25. Specically, Si substrates were cleaned and spin-coated with a 1.2 m layer of S1813 photoresist, then baked at 115 C for 2 min and deposited an 80-nm-thick Au lm using magnetron sputtering. To get suspended Au lm, the sample was immersed in acetone for 24h to fully dissolve the resist and a 100m100m Cu grid was dipped into the solution to pick the lm up, which was then dried by N2 in ultra-clean room to get a at and self-supporting Au lm. Pre-designed patterns were automatically cut by FIB system (FEI helios 600i). Subsequently, the FIB spot was continuously scanned along the bottom edge of the patterned structures, which folded the structures naturally by the ion-implantation induced stress. Through properly controlling the ion dose, a maximum folding angle of 90 could be realized. The acceleration voltage of Ga+ was 30kV. An ion-beam current of 40pA was used for the structure processing.

Transmission spectra were collected by using a 15, 0.4 numerical aperture reective objective lens on an optical microscope (Hyperion 2000) and coupled to a Fourier-transform infrared spectrometer (Vertex 80, Bruker) through a 40m40m spatial aperture. A homemade aperture was inserted

SCIENTIFIC REPORTS

6

www.nature.com/scientificreports/

aer the reective objective to conne the illumination cone with a conical angle of ~5, and the samples were tilted correspondingly to obtain normal incidence during measurement. The transmission spectra were calibrated using air (holes of the grid) as a reference.

The transmission spectra and E-eld distributions of the structures were simulated by using the nite-dierence time-domain (FDTD) method. The E-eld monitors were placed 5 nm above the metal surface. The current distributions were calculated by the commercial soware package CST Microwave Studio based on the nite integration method. We used realistic parameters describing golds lossy properties, with an electric conductivity of 4.561 107 Sm1.The surface current distributions were obtained using an H-eld/surface current monitor.

1. Lukyanchuk, B. et al. The Fano resonance in plasmonic nanostructures and metamaterials. Nat. Mater. 9, 707715 (2010).2. Miroshnichenko, A. E., Flach, S. & Kivshar, Y. S. Fano resonances in nanoscale structures. Rev. Mod. Phys. 82, 22572298 (2010).3. Rahmani, M., Lukyanchuk, B. & Hong, M. H. Fano resonance in novel plasmonic nanostructures. Laser Photonics Rev. 7, 329349 (2013).

4. Wu, C. H. et al. Fano-resonant asymmetric metamaterials for ultrasensitive spectroscopy and identification of molecular monolayers. Nat. Mater. 11, 6975 (2012).

5. Mirin, N. A., Bao, K. & Nordlander, P. Fano Resonances in Plasmonic Nanoparticle Aggregates. J. Phys. Chem. A 113, 40284034 (2009).

6. Fan, J. A. et al. Fano-like Interference in Self-Assembled Plasmonic Quadrumer Clusters. Nano Lett. 10, 46804685 (2010).7. Hao, F. et al. Symmetry Breaking in Plasmonic Nanocavities: Subradiant LSPR Sensing and a Tunable Fano Resonance. Nano Lett.

8, 39833988 (2008).

8. Sonnefraud, Y. et al. Experimental Realization of Subradiant, Superradiant, and Fano Resonances in Ring/Disk Plasmonic Nanocavities. Acs Nano 4, 16641670 (2010).

9. Pryce, I. M., Aydin, K., Kelaita, Y. A., Briggs, R. M. & Atwater, H. A. Highly Strained Compliant Optical Metamaterials with Large Frequency Tunability. Nano Lett. 10, 42224227 (2010).

10. Zhang, Q. et al. Multiple Magnetic Mode-Based Fano Resonance in Split-Ring Resonator/Disk Nanocavities. Acs Nano 7, 1107111078 (2013).

11. Garcia-Vidal, F. J., Martin-Moreno, L., Ebbesen, T. W. & Kuipers, L. Light passing through subwavelength apertures. Rev. Mod. Phys. 82, 729787 (2010).

12. Christ, A., Tikhodeev, S. G., Gippius, N. A., Kuhl, J. & Giessen, H. Waveguide-plasmon polaritons: Strong coupling of photonic and electronic resonances in a metallic photonic crystal slab. Phys. Rev. Lett. 91, 183901 (2003).

13. Hao, F., Nordlander, P., Sonnefraud, Y., Van Dorpe, P. & Maier, S. A. Tunability of Subradiant Dipolar and Fano-Type Plasmon Resonances in Metallic Ring/Disk Cavities: Implications for Nanoscale Optical Sensing. Acs Nano 3, 643652 (2009).

14. Dregely, D., Hentschel, M. & Giessen, H. Excitation and Tuning of Higher-Order Fano Resonances in Plasmonic Oligomer Clusters. Acs Nano 5, 82028211 (2011).

15. Hentschel, M. et al. Transition from Isolated to Collective Modes in Plasmonic Oligomers. Nano Lett. 10, 27212726 (2010).16. Bao, K., Mirin, N. A. & Nordlander, P. Fano resonances in planar silver nanosphere clusters. Appl. Phys. A-Mater. 100, 333339 (2010).17. Hentschel, M., Dregely, D., Vogelgesang, R., Giessen, H. & Liu, N. Plasmonic Oligomers: The Role of Individual Particles in Collective Behavior. Acs Nano 5, 20422050 (2011).

18. Al-Naib, I. et al. Conductive Coupling of Split Ring Resonators: A Path to THz Metamaterials with Ultrasharp Resonances. Phys. Rev. Lett. 112, 183903 (2014).

19. Habteyes, T. G., Dhuey, S., Cabrini, S., Schuck, P. J. & Leone, S. R. Theta-Shaped Plasmonic Nanostructures: Bringing Dark Multipole Plasmon Resonances into Action via Conductive Coupling. Nano Lett. 11, 18191825 (2011).

20. Panaro, S., De Angelis, F. & Toma, A. Dark and bright mode hybridization: From electric to magnetic Fano resonances. Opt. Laser. Eng. 76, 6469 (2016).

21. Verellen, N. et al. Fano Resonances in Individual Coherent Plasmonic Nanocavities. Nano Lett. 9, 16631667 (2009).22. Shaei, F. et al. A subwavelength plasmonic metamolecule exhibiting magnetic-based optical Fano resonance. Nat. Nanotechnol. 8, 9599 (2013).

23. Funston, A. M., Novo, C., Davis, T. J. & Mulvaney, P. Plasmon Coupling of Gold Nanorods at Short Distances and in Dierent Geometries. Nano Lett. 9, 16511658 (2009).

24. Slaughter, L. S., Wu, Y., Willingham, B. A., Nordlander, P. & Link, S. Eects of Symmetry Breaking and Conductive Contact on the Plasmon Coupling in Gold Nanorod Dimers. Acs Nano 4, 46574666 (2010).

25. Cui, A. J. et al. Directly patterned substrate-free plasmonic nanograter structures with unusual Fano resonances. Light-Sci. Appl. 4, e308 (2015).

26. Katsarakis, N., Koschny, T., Kafesaki, M., Economou, E. N. & Soukoulis, C. M. Electric coupling to the magnetic resonance of split ring resonators. Appl. Phys. Lett. 84, 29432945 (2004).

27. Fedotov, V. A., Rose, M., Prosvirnin, S. L., Papasimakis, N. & Zheludev, N. I. Sharp trapped-mode resonances in planar metamaterials with a broken structural symmetry. Phys. Rev. Lett. 99, 147401 (2007).

28. Chen, W. T. et al. Optical magnetic response in three-dimensional metamaterial of upright plasmonic meta-molecules. Opt. Express 19, 1283712842 (2011).

29. Huang, Y. W. et al. Design of plasmonic toroidal metamaterials at optical frequencies. Opt. Express 20, 17601768 (2012).30. Liu, N. et al. Three-dimensional photonic metamaterials at optical frequencies. Nat. Mater. 7, 3137 (2008).31. Ebbesen, T. W., Lezec, H. J., Ghaemi, H. F., Thio, T. & Wol, P. A. Extraordinary optical transmission through sub-wavelength hole arrays. Nature 391, 667669 (1998).

32. Ruan, Z. C. & Qiu, M. Enhanced transmission through periodic arrays of subwavelength holes: The role of localized waveguide resonances. Phys. Rev. Lett. 96, 233901 (2006).

33. Liu, H. T. & Lalanne, P. Microscopic theory of the extraordinary optical transmission. Nature 452, 728731 (2008).34. Georgiou, G., Tserkezis, C., Schaafsma, M. C., Aizpurua, J. & Rivas, J. G. Active loaded plasmonic antennas at terahertz frequencies: Optical control of their capacitive-inductive coupling. Phys. Rev. B 91, 125443 (2015).

35. Kildishev, A. V., Boltasseva, A. & Shalaev, V. M. Planar Photonics with Metasurfaces. Science 339, 6125 (2013).36. Yu, N. F. & Capasso, F. Flat optics with designer metasurfaces. Nat. Mater. 13, 139150 (2014).

This work is supported by the 973 Program of China at Nos 2013CB632704 and 2013CB922404, and the National Natural Science Foundation of China under Grant Nos 61475186, 11434017, 91323304, 11504414, 11574368, 61390503.

SCIENTIFIC REPORTS

7

www.nature.com/scientificreports/

J.F.L. and Z.-Y.L. conceived the idea. Z.G.L. and Z.L. fabricated the structures and performed simulations. Z.G.L., Z.L. and J.F.L. carried out the optical experiments and analyzed the data. J.F.L., W.L., J.J.L., C.G. and Z.-Y.L. supervised the work. All authors participated in the project discussions and manuscript preparation.

Competing nancial interests: The authors declare no competing nancial interests.

How to cite this article: Liu, Z. et al. 3D conductive coupling for efficient generation of prominent Fano resonances in metamaterials. Sci. Rep. 6, 27817; doi: 10.1038/srep27817 (2016).

This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the articles Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/

SCIENTIFIC REPORTS

8