Experimental Demonstration of Electromagnetically Induced Transparency in a Conductively Coupled Flexible Metamaterial with Cheap Aluminum Foil
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We propose a conductively coupled terahertz metallic metamaterial exhibiting analog of electromagnetically induced transparency (EIT), in which the bright and dark mode antennae interact via surface currents rather than near-field coupling. Aluminum foil, which is very cheap and often used in food package, is used to fabricate our metamaterials. Thus, our metamaterials are also flexible metamaterials. In our design, aluminum bar resonators and aluminum split ring resonators (SRRs) are connected (rather than separated) in the form of a fork-shaped structure. We conduct a numerical simulation and an experiment to analyze the mechanism of the proposed metamaterial. The surface current due to LSP resonance (bright mode) flows along different paths, and a potential difference is generated at the split gaps of the SRRs. Thus, an LC resonance (dark mode) is induced, and the bright mode is suppressed, resulting in EIT. The EIT-like phenomenon exhibited by the metamaterial is induced by surface conducting currents, which may provide new ideas for the design of EIT metamaterials. Moreover, the process of fabricating microstructures on flexible substrates can provide a reference for producing flexible microstructures in the future.
KeywordsElectromagnetically induced transparency Terahertz Metamaterial Surface currents Potential difference
Electromagnetically induced transparency
Split ring resonators
Localized surface plasmon
- Q factor
Terahertz time domain spectroscopy
Metamaterials [1, 2] are artificially engineered composites with subwavelength structures. Their physical properties, such as the dielectric constant, permeability, and conductivity, can be arbitrarily designed by changing the structure and size of the periodic lattice Therefore, many interesting phenomena can be realized by tailoring the geometry of the unit cells, with immense application potential such as metalenses and related wavefront regulation in metasurface [3, 4, 5, 6, 7, 8], negative index media [9, 10], polarizers [11, 12], metamaterial absorbers [13, 14, 15], and reconfigurable metadevices . The combination of metamaterials and two-dimensional materials further widens the research scope [17, 18, 19]. Among them, the analog of electromagnetically induced transparency (EIT) exhibited by metamaterials is a research hotspot.
EIT  is a quantum-mechanical phenomenon originally observed in atomic or molecular systems based on destructive interference between transitions driven by two laser beams. EIT renders a highly opaque medium, transparent over a narrow spectral region because of the lack of absorption, which is now realized in waveguide structures [21, 22]. On the other hand, the analog of EIT is also observed in metamaterials, characterized by a relatively narrow transparent peak in a wide opaque region in the spectrum. Various resonances can occur in metamaterials because of the interaction between the periodic structures and the incident electromagnetic field. Furthermore, the destructive interference between the different resonances causes EIT-like phenomena in metamaterials. Many researchers are now engaged in this topic, and a variety of structures has been proposed to realize this phenomenon. The current common EIT-forming mechanism is based on the destructive interference between “bright modes” and “dark modes”. For example, the inductive-capacitive (LC) oscillation in metallic split ring resonators (SRRs) suppress the localized surface plasmon (LSP) resonance in metallic bars [23, 24, 25, 26]; quadrupole suppress dipole wherein metamaterials combined with bar-shaped resonators [27, 28, 29, 30] or bar-shaped grooves [31, 32] in different directions; the magnetic resonance in a dielectric block or a dielectric ring resonator suppresses the electrical resonance in a dielectric bar resonator [33, 34, 35]. The destructive interference between a bright mode with a lower quality factor (Q factor) and a bright mode with a higher Q factor (also known as a quasi-dark mode) also induces analog of EIT in metamaterials . For instance, LC resonances with a higher Q factor in SRRs suppress the LSP resonances with a lower Q factor in metallic ring resonators [37, 38, 39]; a guide mode with a higher Q factor in a waveguide layer suppresses the resonances in a periodic structure above the waveguide layer [40, 41, 42]. Some scholars incorporated controllable substances in the design to realize all-optical tuning of EIT [43, 44] or active electronic controlling of EIT [45, 46]. In most designs, particularly in metallic metamaterials, antennae with different modes are always separated; they interact with each other through near-field coupling.
A metal has a high electrical conductivity in the terahertz band. Moreover, a metallic metamaterial structure is subjected to surface plasmon when the resonance is excited, and a surface conduction current is induced at the same time, which makes conductively coupling possible [47, 48, 49]. Here, we propose a design wherein different resonators interact via surface currents. We propose a conductively coupled terahertz metallic metamaterial, in which the bright and dark mode antennae are connected in the form of a fork-shaped structure to realize analog of EIT.
The periods of the unit cells are equal in both the x and y directions; Px = Py = 150 μm. The length of the square SRR is a = 45 μm. The gap between the two SRRs is S = 30 μm. The slit gap of the SRR is g = 10 μm. The length of the aluminum bar is L = 65 μm. The line width of the aluminum strips and SRRs is w = 8 μm. The substrate is made of polyethylene terephthalate (PET). For all the simulations, corresponding full-wave simulations were carried out using CST Microwave Studios (the metal selected was aluminum with a conductivity of 3.56 × 107 S/m, and the permittivity of the PET substrate is 3.2). The thickness of the aluminum structure was set to 150 nm in the simulation. We assumed the incident light to be a plane wave propagating in the opposite direction of the z-axis. The electric and magnetic fields of the incident light are polarized along the y- and x-axes, respectively.
As for the experiment, we used the purchased composite of a PET-aluminum film as the raw material. This kind of commercial aluminum foil is very cheap and often used in common food package. Lithography (laser direct writing) and wet etching processes were employed in fabrication. Compared with conventional micro/nanofabrication technologies, laser direct writing technique offers several distinct advantages, such as designable processing without the use of masks, ease of integration with given devices, and feasibility of 3D structuring capability . As the PET substrate is very soft owing to its thickness of approximately 20 μm, we first added some volatile liquid on a flat and clean quartz substrate, then flattened the PET–aluminum film composite on the quartz substrate, and discharged the air between the composite material and the quartz substrate. After the liquid evaporates, the flat composite firmly attaches onto the surface of the quartz substrate; this is convenient for the subsequent spin-on photoresist and photolithography processes.
Results and Discussion
First of all, metamaterial structure is composed of aluminum. It is well known that the metal aluminum surface is prone to form a dense oxide film, which leads to the reduction of the conductivity of the structure and weakens the conductively coupling effect of the structure. The effect of conductivity on metamaterial EIT phenomenon is shown in Fig. 4a. As the conductivity decreases (from 3.56 × 107 S/m to 3.56 × 105 S/m), the EIT amplitude decreases significantly, and the frequency shifts slightly, from 0.76 to 0.72 THz. In addition, the size of the fabricated metamaterials has also been measured with a microscope. It is found that there are some differences between the size of the fabricated structure and the parameter setting in the simulation process. Here, we list some obvious difference: the line width of the aluminum strips and SRRs, w, (6.5~7.5 μm) is thinner than the designed value (8 μm), and the length of the square SRR, a, (43~41 μm) is smaller than the designed value (45 μm), the length of the aluminum bar, L, (61~62 μm) is shorter than designed value (65 μm). The influences of w, a, and L on EIT effect are shown in Fig. 4b, c respectively. As shown in the Fig. 4b, as the w decreases, the frequency of the EIT phenomenon decreases. Since the parameter w involves both the SSRs and the metal bar structure, the change of this parameter causes the shift of the absorption frequency and the transmission frequency of the EIT. While in Fig. 4c, d, as the a and L decrease, the transmission peak and the absorption range of the EIT phenomenon appear blue shift respectively, that is, the frequency increases. The combination of all these differences in experiment and simulation ultimately led to the difference between the actual measured spectrum and the simulated spectrum. What’s more, according to the frequency shift of the absorption region and the transmission peak caused by the variation of parameters in Fig. 4, it can also be concluded that although the bright and dark mode antennas are integrated in the structure, there are also strict requirements for the size of both antennas to make these two frequencies of modes matched with each other.
Figure 5b shows the surface current distribution at the EIT frequency (0.76 THz). The vortex surface current is mainly concentrated at the SRRs, indicating a fundamental LC resonance and LSP resonance suppression. As for the second transmission dip at a higher frequency (0.81 THz), the surface current distribution is from one end to the other end along the y-axis direction, indicative of an LSP resonance, as shown in Fig. 5c. However, the surface current flows through the inner metallic arm of the SRRs. In comparison with the path, shown in Fig. 5a, the conduction path of the surface current, shown in Fig. 5c, is shorter, which corresponds to a shorter resonance wavelength and a higher resonance frequency. Figure 5e, d, and f show the electric field distributions at the frequencies of the EIT transmission peak and two transmission dips besides the EIT peak. In Fig. 5e, the electric field energy is mainly concentrated at the gaps of the SRRs, whereas in Fig. 5d and f, the electric field energy is mainly concentrated at the two ends of the structure. These phenomena correspond to their respective surface current distributions.
However, if the points connecting the bar resonator and the SRRs are located on the vertical center line of the SRRs, as shown in Fig. 6b, the two paths on the outer side and the inner side after the bifurcation are symmetrical. In this case, R1’ = R3’, L1’ = L3’. Therefore, the speed of charging and discharging along the two paths is always the same, and there is no potential difference.
As for the frequency of this LSP resonance (0.87 THz), it is higher than that of previous structure. It is because in the current structure, the surface current can flow through two conduction paths. This is equivalent to a parallel circuit where the resistance and the inductance are smaller than any one of the branches. This is the same as the effect of passing through a shorter conduction path. The conduction path becomes shorter, the resonance wavelength becomes smaller, and the resonance frequency becomes higher.
In Fig. 8b, when the connecting bar in the middle is bent, which is to prepare for the movement of the connecting point toward outside, the frequency of absorption region of the EIT becomes higher with the increasing of the bending angle. When the bending angle increases, more parts of the conduction path are connected in parallel, i.e., conduction path becomes wider, which is the same as the effect of passing through a shorter conduction path. The conduction path becomes shorter, the resonance wavelength becomes smaller, and the resonance frequency becomes higher. This also explains why the resonant frequency in Fig. 7 is higher than that in Fig. 3. In Fig. 8c, when the joint point moves outward, the asymmetry decreases, the charge and discharge speeds of the C1 along the two paths tend to be the same; the potential difference becomes smaller, and the intensity of the dark mode gradually becomes weaker, leading to the decline of the transmission peak of EIT. This also reflects that the greater difference between the two paths along the SSR after bifurcation from the connection point, the stronger the effect of EIT.
Although the direction is different, the overall trend in the surface current is considered the same, because the incident electromagnetic field is oscillating back and forth. Figure 9b shows the spectra of the SRR combination under incident light excitation with different polarization. When the electric field is polarized perpendicular to the direction of the split gap, no resonance occurs in the range of 0.5–1 THz, and the transmission remains at a high level. When the electric field is polarized parallel to the gaps of the SRRs, a resonance is generated at 0.78 THz. Figure 9e shows the surface current distribution when this resonance is excited. The surface current circulates back and forth on the surface of the SRRs, similar to the distribution shown in Fig. 5b. However, the flow direction of the two vortex surface currents, in Fig. 5b, is mirror-symmetric to the y-axis, whereas the vortex surface currents, in Fig. 5e, are in the same direction. This is because, in Fig. 9e, the resonances of the two SRRs are induced by the same electric field. Therefore, the direction of the vortex surface current is the same. However, in Fig. 5b, both the structure of the proposed metamaterial and the directions of the potential difference generated at the split gaps of the two SRRs are mirror-symmetric to the y-axis, thus making the excited surface current mirror-symmetric to the y-axis as well. The difference in the frequencies (0.76 THz vs. 0.78 THz) can be attributed to the fact that the vortex surface current in the conductive metamaterial is not strictly distributed only in the SRRs, and the elongation in the conduction path leads to an increase in the resonant wavelength, thereby making the frequency of the EIT peak (0.76 THz) slightly lower than the LC resonance frequency of the SRR combination (0.78 THz). As shown in Fig. 9c, the combined structure of the metal bar and the inner part of the SRRs produces a significant resonance at 0.79 THz under an electric field excited along the y-axis. Figure 9f shows the surface current distribution when the resonance of this structure is induced, exhibiting a typical LSP resonance. The resonances of the abovementioned components correspond to the conditions of the low-frequency transmission dip, the EIT transmission peak, and the high-frequency dip, respectively.
In conclusion, we proposed a conductively coupled terahertz metallic EIT metamaterial, in which the bright and dark mode antennae are connected in the form of a fork-shaped structure. Aluminum foil, which is very cheap and often used in food package, is used to fabricate our metamaterials. Numerical and experimental analyses were conducted to analyze its mechanism. The surface current due to LSP resonance (bright mode) flows along different paths. Because of the asymmetry of the connection point with respect to the slit gap of the SRR, a potential difference is generated at the gaps of the SRRs. This is equivalent to an external electromagnetic field excitation with the electric field polarized along the slit gap. Thus, an LC resonance (dark mode) is induced, and the bright mode is suppressed, resulting in EIT. The proposed structure interacts via surface conducting currents. This may provide new ideas for the structural design of EIT metamaterials. Moreover, the process of fabricating microstructures on flexible substrates can provide a reference for producing flexible microstructures in the future.
We thank the Centre for THz Research, China Jiliang University for the use of their equipment.
Jie Hu conceived the research, conducted simulations, experiment and analyses, and wrote the manuscript. Tingting Lang supervised the whole work. Zhi Hong assisted in the analysis. Weihang Xu and Jianjun Liu assisted in fabrication of metamaterials and experimental measurement. All the authors reviewed the manuscript. All authors read and approved the final manuscript.
This work was supported by the National Natural Science Foundation of China (No. 61875251, No. 61875179).
The authors declare that they have no competing interests.
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