Realization of Multifunctional Metamaterial Structure Based on the Combination of Vanadium Dioxide and Graphene

Abstract

Combining tunable properties and various functionalities into a single metamaterial structure has become a novel research hotspot and can be used to tackle great challenges. The multifunctional metamaterial structure that combines absorption, linear-to-circular (LTC) polarization conversion, filtering and switching functions into a single metamaterial device was designed and investigated in this study. The switching of different functions can be achieved based on the phase transition of vanadium dioxide (VO₂) and change of graphene chemical potential. When VO₂ is in a metal state, the multi-frequency absorption and LTC polarization conversion can be achieved with different chemical potentials. When VO₂ is in the insulator state and the polarization angle of incident wave is 45°, the device can be used to select or isolate the incident waves with different polarization states in the frequency region of 1.2–1.8 THz. Furthermore, when the chemical potentials are 0.05 eV and 1.2 eV, the corresponding transmissions of the TE-polarized wave demonstrate the opposite results, realizing the switching functions in the frequency region of 0.88–1.34 THz. In the frequency region above 2 THz, the multi-frequency rejection filter can be achieved. The designed switchable multifunctional metamaterial device can be widely implemented in radar monitoring and communication systems.

1. Introduction

Modulating the terahertz waves is particularly important in responding to the increasingly complex electromagnetic environment and communication needs. The absorber, polarization converter, and filter are especially essential devices in the fields of wave modulation. Metamaterials are artificially designed electromagnetic materials that are formed by periodic distribution of subwavelength microstructures. Traditional metamaterial devices, including absorbers, polarization converters, filters, etc., are usually designed for realizing a single function. In recent years, with the introduction of functional materials such as graphene, VO₂, liquid crystal, etc., the ability to design multifunctional metamaterial structures has become one of the main research hotspots [1,2,3,4,5,6,7,8,9,10]. Among these materials, graphene can provide the excellent electrical properties, including strict field confinement, high electron mobility, flexibility, and tuning properties [11]. Graphene-based metamaterial devices enable efficient dynamic modulation, since the graphene conductivity can be dynamically modulated by changing the chemical potential through electrical stimulating or chemical doping [12]. One method to realize function reconfiguration is to introduce the graphene materials into the metamaterial structures. In addition, VO₂ is a kind of phase-change material that performs the reversible transition from the insulating phase to the metal phase excited by the electric field, temperature field, and light field. Thus, VO₂ enables the switchable and tunable functionalities for smart devices since the conductivity is capable of 4–5 orders of magnitude change, and the phase-change process can be realized in several picoseconds [13]. Inspired by the above extraordinary properties, VO₂ can be used as a promising candidate in several advanced devices, such as optical switches, modulators, absorbers, and polarization converters.

Advances toward the combination of VO₂ and graphene in multifunctional metamaterial structures have been put forward. By combing the VO₂ and graphene, Zhu et al. designed a switchable terahertz metamaterial structure to realize wide-band and multi-band absorption [14]. Liu et al. demonstrated a metamaterial absorber by treating the VO₂ and graphene to realize dynamically tunable dual-wide-band absorption [11]. When the VO₂ switches from the metallic phase to the insulator phase, the operation frequency can be changed from the high-frequency to low-frequency region accordingly. By altering the Fermi energy level of graphene, its absorptivity can be continuously varied from 5.2% to 99.8%. Zhao et al. proposed a dynamically switched wide-band metamaterial polarization converter by treating the VO₂ and graphene gratings in terahertz region [15]. The phase transition of VO₂ enables the polarization conversion switching between transmissive and reflective modes, and the introduction of double-layer graphene grating should improve the transmittance. Tang et al. designed a multifunctional terahertz metamaterial structure based on the hybrid VO₂-graphene integrated structure [16]. Enabled by the phase transition of VO₂, the asymmetric transmission and two different polarization conversions can be integrated into one device in the terahertz region. Wang et al. realized a dual-functional tunable wide-band absorber/reflector based on the periodic cross-shaped graphene array and a VO₂ layer [17]. Most of the reported studies have focused on achieving similar functionality in a single device by using a combination of VO₂ and graphene.

Within the investigation of this study, we aimed to design a multifunctional metamaterial structure based on the manipulability of the chemical potential of graphene and the phase-transition properties of VO₂ material. Compared to the previously reported metamaterial devices, the proposed scheme here can provide three main advantages, which are as follows: (1) different functions, including multi-frequency absorption and linear-to-circular (LTC) polarization conversion, and different transmission characteristics can be integrated into a single metamaterial structure; (2) when VO₂ is in the metal state, the designed structure works in reflection mode, and the functions of the metamaterial structure can switch between absorption (µ_c = 1.2 eV) and LTC polarization conversion (µ_c = 0.05 eV) by varying the graphene chemical potential; (3) when VO₂ is in the insulator state, the structure works in the transmissive mode, which exhibits different transmission characteristics for different incidences. In addition, the effects of several structure geometrical parameters on the performances have also been investigated. The proposed scheme may pay a new route in designing tunable and switchable multifunctional terahertz metamaterial structures.

2. Materials and Methods

Figure 1 gives the structural diagram of the proposed hybrid VO₂–graphene-integrated metamaterial structure, which is arranged periodically in the x- and y-direction. The unit cell of the proposed metamaterial structure is composed of five layers from top to bottom: metal split ring resonator, SiO₂ spacer, metal split ring resonator, SO₂ spacer, and VO₂ layer. As depicted in Figure 1, the structure sizes of the unit cell are p_x = p_y = 80 µm, t₁ = 0.2 µm, t₂ = 24 µm, t₃ = 13 µm, R₁ = 30 µm, R₂ = 27 µm, and α = 5°. The top and middle metal split rings are 0.2 µm–thick gold microstructures with a conductivity of 4.561 × 10⁷ S/m [18]. The gaps of the two metal split rings are arranged vertically, and the gaps are filled with graphene material with a thickness of 1 nm [18]. In the investigation, the dielectric layers are SiO₂ material with a dielectric constant of ε_r = 3.75 [15] and electric tand. of 0.0004. The conductivity of graphene and VO₂ can be varied by using voltage and temperature, respectively.

The fast-developing micro–nano-fabrication technology can be used to fabricate the designed multifunctional structures [15]. The designed metamaterial device can be manufactured by using the techniques in the related references [19,20,21].

In the terahertz frequency region, the surface complex conductivity of graphene, σ_g = σ_intra + σ_inter, can be characterized by the intra-band conductivity, σ_intra, and the inter-band conductivity, σ_inter [22,23]:

$${\sigma }_{\mathrm{intra}}=-j\frac{e^2{k}_{\mathrm{B}}T}{\pi {ħ}^2(\omega -j2\mathsf{\Gamma })}\left(\frac{{\mu }_{\mathrm{c}}}{k_{\mathrm{B}}T}+2\ln \left(e^{-\frac{{\mu }_{\mathrm{c}}}{k_{\mathrm{B}}T}}+1\right)\right)$$

(1)

$${\sigma }_{\mathrm{inter}}=-j\frac{e^2}{4\pi ħ}\ln \left(\frac{2\left|{\mu }_{\mathrm{c}}\right|-(\omega -j2\mathsf{\Gamma })ħ}{2\left|{\mu }_{\mathrm{c}}\right|+(\omega -j2\mathsf{\Gamma })ħ}\right)$$

(2)

where ω represents the angular frequency of the incident terahertz wave, µ_c represents the chemical potential or Fermi level of graphene [15], T denotes the temperature, e represents the electronic charge, k_B denotes the Boltzmann constant, Γ = ħ/2π denotes the phenomenology scattering rate, ħ represents the reduced Plank constant, τ = µµ_c/(e$v_{\mathrm{f}}^2$) represents the relaxation time, and here τ = 0.2 ps is used in our study [24,25]. Moreover, v_f = 1.1 × 10⁶ m/s represents Fermi velocity, and μ represents the carrier mobility, which is mainly influenced by the graphene doping degree or its own defects at room temperature [26]. The surface conductivity of monolayer graphene is affected by the chemical potential variations caused by the chemical doping [27] or bias voltage stimulating [28]. Based on the Pauli exclusion principle, the σ_inter can be ignored when ħω << µ_c and k_BT << µ_c [29]. Thus, the surface conductivity, σ_g, of graphene can be simply expressed as the Drude model [23]:

$${\sigma }_{\mathrm{g}}\approx \frac{e^2{\mu }_{\mathrm{c}}}{\pi {ħ}^2}\frac{j}{\omega +j/\tau }$$

(3)

The effective permittivity, ε_g, of the graphene can be described by ε_g = 1 + jσ_g/(ε₀ωd_g) [18,30], where ε₀ represents the vacuum permittivity, and d_g denotes the thickness of the graphene material, which is set as 1 nm in the investigation [18].

Besides graphene, VO₂ is one of the important phase-transition materials. In general, the permittivity of VO₂ in the terahertz region can be characterized by using the Drude model [31]:

$${\epsilon }_{\mathrm{V}{\mathrm{O}}_2}={\epsilon }_{\infty }-\frac{{\omega }_p^2({\sigma }_{\mathrm{V}{\mathrm{O}}_2})}{{\omega }^2+i\gamma \omega }$$

(4)

where ε_∞ = 12 represents the permittivity at infinite frequency; γ = 5.75 × 10¹³ rad/s. ω_p(${\sigma }_{{\mathrm{VO}}_2}$) represents the plasma frequency; and ${\omega }_p^2$(${\sigma }_{{\mathrm{VO}}_2}$) = ${\sigma }_{{\mathrm{VO}}_2}$/(${\sigma }_{{\mathrm{VO}}_2}$${\omega }_p^2$(σ₀)), where ω_p(σ₀) = 1.4 × 10¹⁵ rad/s. To simulate the insulating-metal phase change characteristics of VO₂, different conductivities are used to characterize the different optoelectronic characteristics of VO₂. In this study, ${\sigma }_{{\mathrm{VO}}_2}$ = 3 × 10⁵ S/m and ${\sigma }_{{\mathrm{VO}}_2}$ = 10 S/m [32] were used to represent the metallic and insulator states of VO₂, respectively. The conductivity of VO₂ can be changed by laser radiation, external bias voltage, and thermal control.

The metamaterial device was designed and the related simulations were performed by using the finite difference time-domain method. The unit cell boundary conditions are used in x and y axes to mimic the infinite arrays, and the open boundaries are applied in the z axis. Linearly and circularly polarized terahertz waves transmitting along the -z direction are incident on the metamaterial structure.

3. Results and Discussions

The operation characteristics of the designed multifunctional metamaterial unit cell structure were studied, and the electromagnetic responses of different functions were achieved. By combining the phase transition of VO₂ and variation of graphene chemical potential, different functions can be integrated into a single metamaterial structure. When VO₂ is in the metallic state (${\sigma }_{{\mathrm{VO}}_2}$ = 3 × 10⁵ S/m), according to different chemical potentials, the designed structure can exhibit linear-to-circular (LTC) polarization conversion properties (µ_c = 0.05 eV) and absorption properties (µ_c = 1.2 eV), respectively. In 2017, Bezares et al. presented FeCl₃-intrcalated graphene as a new plasmonic material with high stability under environmental conditions and carrier concentrations, corresponding to a Fermi energy of 1.21 eV on the two-monolayer sample and 1.4 eV for the bilayer graphene [33]. By use of the electrolyte gate technique, for example, carrier densities as high as n = 4 × 10¹⁴ cm⁻² have been obtained for electrons and holes [34], and the corresponding chemical potential is about 1.17 eV [35]. A reasonable tuning range of the chemical potential can reach 1.2 eV based on the current situation that a carrier density of up to 10¹⁴ cm⁻² has been realized in experiments [36,37]. When VO₂ is in the insulator state (${\sigma }_{{\mathrm{VO}}_2}$ = 10 S/m), the designed metamaterial structure can act as a filter, as well as a switch.

3.1. Designed Metamaterial Structure Works as the Polarization Converter

When the conductivity of VO₂ layer is ${\sigma }_{{\mathrm{VO}}_2}$ = 3 × 10⁵ S/m, the VO₂ layer acts like a metal that prevents the transmission of incident terahertz waves. In this case, when the chemical potential of graphene is set to µ_c = 0.05 eV, the designed metamaterial structure can be used as an LTC polarization converter, which is illuminated by the TE-polarized (electric field polarized along the y axis) or TM-polarized (electric field polarized along the x axis) incident terahertz waves with a polarization angle of 0°. In the x–y-coordinate system, for realizing the LTC polarization conversion, the reflection coefficients for co-polarization (TE-to-TE), r_EE, and cross-polarization (TE-to-TM), r_ME, should be equal, providing a phase difference of Δφ = φ_ME − φ_EE = 2nπ ± π/2 (n represents an integer), and “−” and “+” define the left-handed and right-handed circularly polarized terahertz waves [38,39]. As given in Figure 2a,b, in the frequency bands of 0.64–1.28 THz and 1.54–1.85 THz, the reflection coefficients exhibit approximately the same intensity, and the corresponding phase difference is around 90° (or −270°) and −90°. Thus, the reflective wave can be regarded as the right-handed circularly polarized (RHCP) wave and left-handed circularly polarized (LHCP) wave in the corresponding frequency region. To quantify the performance of the designed metamaterial structure, Stokes parameters (S) are used to evaluate the efficiency of the LTC polarization conversion. The expressions of the Stokes parameters are as follows [40]:

$$S_0=|r_{EE}{|}^2+|r_{ME}{|}^2$$

(5)

$$S_1=|r_{EE}{|}^2-|r_{ME}{|}^2$$

(6)

$$S_2=2\left|r_{EE}\right|\left|r_{ME}\right|\cos (\Delta \phi )$$

(7)

$$S_3=2\left|r_{EE}\right|\left|r_{ME}\right|\sin (\Delta \phi )$$

(8)

The normalized ellipticity of χ = S₃/S₀ is further given to evaluate the polarization conversion degree. Specifically, χ = −1 and χ = +1 indicate that the reflective wave is a LHCP wave and RHCP wave, respectively. Figure 2c depicts the relationship between the normalized ellipticity and the operating frequency. The results demonstrate that the ellipticity approaches 1 within the frequency range of 0.64 to 1.28 THz (ellipticity above 0.85), which further confirms that the reflective wave can be estimated as RHCP wave. In addition, in the frequency range of 1.54 to 1.85 THz, the ellipticity approaches −1 (below −0.85), indicating that the reflective wave can be regarded as the LHCP wave.

In addition, we define sin(2β) = S₃/S₀ and introduce the axis ratio AR = 10log(tanβ) to evaluate the circular polarization characteristics [41], where β represents the ellipticity angle. As shown in Figure 2d, the AR value is lower than 3 dB in the frequency bands of 0.64 to 1.28 THz and 1.54 to 1.85 THz, demonstrating that the proposed structure realizes good LTC polarization conversion operation properties. The energy conversion efficiency is calculated by using the equation η = |r_ME|² + |r_EE|². The efficiency of the RHCP is higher than 0.8, and that of the LHCP is larger than 0.7. The results demonstrate that the designed metamaterial structure can realize the high-efficiency conversion operation.

In general, the geometry parameters of the metamaterial device have an effect on the operation performances. In addition, errors can be introduced in the structural dimensional parameters during the device processing. Therefore, the geometric parameters of the metamaterial structure were also investigated. The variations of the ellipticity spectrum of the LTC polarization conversion structure with the geometry parameters (R₂ and t₂) were studied when the other parameters are fixed as initial settings, and the results are given in Figure 3. From Figure 3a, we can see that, when the value of R₂ rises from 25 to 29 µm, the ellipticity of RHCP wave increases. At the same time, the corresponding bandwidth narrows slightly, which is caused by the red-shift of the overall LHCP frequency band with the augment of R₂. Furthermore, as given in Figure 3b, the overall ellipticity spectrum exhibits a slight red-shift trend with the augment of t₂. The above results demonstrate that the variation of geometric parameters have a certain influence on the operating characteristics, but the influence is acceptable according to the fabricating error.

3.2. Designed Metamaterial Structure Works as the Absorbers

Using the above metamaterial structure operating at reflection mode (${\sigma }_{{\mathrm{VO}}_2}$ = 3 × 105 S/m), when the chemical potential of graphene is assumed to be 1.2 eV, the metamaterial device is able to obtain selective absorption of linearly and circularly polarized incident terahertz waves. Thus, the metamaterial device can achieve the multi-frequency absorption. Firstly, we demonstrate the absorption operation of the metamaterial structure under linear polarization incident. It should be noted that the results exhibit the same response for the TM-polarized terahertz waves incidence because of the symmetry of the structure. The absorption, A, of the designed metamaterial structure can be calculated from the expression A = 1 − R − T − R_⊥. In the above expression, R = |S₁₁|² and T = |S₂₁|² represent the reflection and transmission, respectively. Moreover, the parameter R_⊥, indicating the reflection of cross-polarized wave, also needs to be taken into account [42]. In the investigation, on the basis of the calculation results illustrated in Figure 4a, the transmission T and cross-polarized reflection R_⊥ can be neglected. The TE-polarized incident terahertz wave exhibits three absorption peaks at 0.89 THz, 1.78 THz, and 3.31 THz, and the corresponding absorptivity values of the three peaks are 96.77%, 90.14% and 97.44%, respectively. When the incident electric field is along the y direction, the strong electric polarization can be first caused, forming an electric dipole resonance. Then the incident waves enter the SiO₂ layer, and the ground metallic phase VO₂ film induces destructive interference that resembles the Fabry–Perot resonant effect, leading to a huge energy dissipation of the incoming terahertz wave.

When the terahertz wave is vertically incident on the metamaterial structure’s surface, the intrinsic mechanism for the operation of metamaterial absorber can be explained by using the impedance matching theory. The real and imaginary parts of the relative impedance of the metamaterial absorber can be derived based on the S parameters. The expressions of the relative impedance are as follows [9]:

$$A=1-R=1-{\left|\frac{Z-Z_0}{Z+Z_0}\right|}^2=1-{\left|\frac{Z_r-1}{Z_r+1}\right|}^2$$

(9)

$$Z_r=\pm \sqrt{\frac{{(1+S_{11})}^2-S_{21}^2}{{(1-S_{11})}^2-S_{21}^2}}$$

(10)

where Z₀ and Z represent the effective impedances in air and in the metamaterial device, respectively. Moreover, Z_r = Z/Z₀ represents the relative impedance between the air and the metamaterial device. The absorption of the metamaterial device reaches the maximum values when the impedance of the device is equal to the impedance in the air, meaning that the relative impedance, Z_r, of the structure is equal to 1. As demonstrated in Figure 4b, the real part is gradually approaching 1, while the imaginary part is gradually approaching 0 at the corresponding high absorption resonant peaks, indicating that the effective impedance of the structure and the air gradually match each other. It should be noted that, when the LHCP or RHCP terahertz waves are incident on the device, the absorption performances of the device are similar to the linearly polarized incidence (not shown in the paper).

Next, the absorption properties of the multi-band metamaterial absorber with different polarization angles are studied. Figure 5 depicts the absorption versus frequency as the polarization angle rises from 0° to 90° in a step of 5°. The results demonstrate that the operation responses of the proposed multi-band metamaterial absorber with TE-polarized normal incidence do not change with the variation of the polarization angle, and the absorption spectra are highly coincident. The insensitivity to the polarization angle is caused by the symmetry structure of the unit cell in the x and y axes, and it is very helpful in many practical applications.

In addition, we also discussed the effects of the geometric parameters of t₂ and R₂ on the absorption performances. As illustrated in Figure 6a, with the increase of t₂, the frequency bands around 1.78 THz and 3.35 THz show a slight red-shift trend. From Figure 6b, we can see that, when R₂ rises from 25 to 29 µm, the frequency band around 1.7 THz illustrates a more obvious change in the absorption performance than that of the other frequency bands. Moreover, the overall absorption spectrum demonstrates a red-shift trend.

3.3. Designed Metamaterial Structure Acts as a Filter

When the conductivity of VO₂ is 10 S/m and the chemical potentials of graphene are 0.05 and 1.2 eV, the designed metamaterial structure is able to act as a filter, which performs different filtering responses for TE- and TM-polarized incident terahertz waves with the polarization angle of 45°. The device contains a top layer pattern combining metal split ring and graphene filled in gaps, a first lossy SiO₂ dielectric layer, a middle layer pattern with the same structure as the top layer, a second lossy SiO₂ dielectric layer, and a base VO₂ dielectric layer. For different graphene chemical potential values, the responses related to the TE- and TM-polarized terahertz waves are different. When the chemical potential is µ_c = 0.05 eV, the TE-polarized terahertz waves and TM-polarized terahertz waves have completely different transmission rates in the low frequency band, as depicted in Figure 7a. In the frequency band of 1.2–1.8 THz, the maximum transmission of the TE-polarized incident wave is higher than 80%, while the value of the TM-polarized incident wave is lower than 20%. This phenomenon can be used to distinguish the incident terahertz waves with different polarization states and can also act as an isolator for incident waves with different polarization states. In the frequency region higher than 2 THz, the high transmission of 83.8% and 94% can be achieved at the center frequencies of 2.19 and 2.42 THz for the TE-polarized incident wave, and the high transmissions of 93.4%, 86%, and 89% can be achieved at the center frequencies of 2.2, 2.47, and 2.62 THz for the TM-polarized incident wave, respectively. In addition, at the resonance frequencies, f_c, of 2.25 THz (TE-polarization), 2.34 THz (TM-polarization), and 2.54 THz (TM-polarization), the corresponding transmissions of the proposed metamaterial structure are 3.2%, 2.1%, and 5.8%, demonstrating good stop-band characteristics. The corresponding stop-band bandwidths ∆f(−3 dB) are 120, 140, and 50 GHz, and the corresponding quality factors, Q = f_c/∆f, are 18.75, 16.71, and 50.8. Moreover, the transmission properties can also enable the construction of a terahertz wave sensor, and the related investigation method can be found in our previous work [43].

When the chemical potential is µ_c = 1.2 eV, the TE-polarized terahertz waves and TM-polarized terahertz waves exhibit similar transmission responses in the low frequency region, as given in Figure 7b. In the high frequency range, the TE- and TM-polarized incident waves have a notch resonant frequency point, with the transmission values of 17% (2.22 THz) and 18% (2.56 THz), respectively. For TE-polarized incident wave, the designed structure can provide switching functions in a specific frequency range, as illustrated in Figure 7c. In the low frequency region, when the chemical potentials are 0.05 and 1.2 eV, the corresponding transmissions of the TE-polarized wave demonstrate the opposite results, leading to the realization of switching function. When µ_c is 1.2 eV, the transmittance of TE-polarized incident wave is lower than 10% in a narrow frequency range (0.88–1.34 THz). It should be noted that the bandwidth can be broadened by further optimization, including changing the structure size and material properties, etc. In practical applications, specific functions can be implemented according to the requirements. In the high frequency range, when µ_c augments from 0.05 to 1.2 eV, the metamaterial structure changes from a multi-frequency rejection filter to a single-frequency rejection filter. As given in Figure 7d, for TM-polarized incident wave, when µ_c rises from 0.05 to 1.2 eV, the structure also changes from a multi-frequency rejection filter to a single-frequency rejection filter.

In addition, the influences of geometric parameters (t₂ and R₂) on the filtering characteristics were also investigated. The conductivity of VO₂ and chemical potential of graphene are ${\sigma }_{{\mathrm{VO}}_2}$ = 10 S/m and µ_c = 0.05 eV, respectively, and the polarization angle of incident wave is 45°. As given in Figure 8a,b, in the low frequency region (below 2 THz), the changes of t₂ result in only a slight effect on the transmission intensity. In the high frequency band, the change of t₂ can affect the position of the resonant peaks, causing the transmission spectrum to show a red-shift trend with the augment of t₂. As illustrated in Figure 8c, for the TE-polarized incident wave, when the R₂ rises from 25 to 29 µm, the transmission of the frequency band 1.2–1.8 THz gradually increases, and the frequency band has a red-shift trend. In Figure 8d, the transmission of the TM-polarized incident wave in the frequency band 1.2–1.8 THz slightly increases with the increase of R₂, and the position of the notch resonant frequency does not change significantly. The results demonstrate that the above transmission functions can also be realized when the geometric parameters perform a slight variation.

4. Conclusions

In conclusion, we proposed a novel kind of multifunctional metamaterial structure based on the combination of VO₂ and graphene materials that performs the absorption, LTC polarization conversion, filtering, and switch functions in a single metamaterial device. The integration of different functions into a single metamaterial device was realized by using the insulator–metal phase transition of VO₂ and variation of graphene chemical potential. When VO₂ is in metal state and the chemical potential is 0.05 eV, the RHCP and LHCP can be achieved in the frequency bands of 0.64–1.28 THz and 1.54–1.85 THz, respectively. When the chemical potential rises from 0.05 to 1.2 eV, three absorption peaks at 0.89, 1.78, and 3.31 THz with the corresponding absorptivity of 96.77%, 90.14%, and 97.44% can be obtained. When VO₂ is in insulator state and the polarization angle of incident wave is 45°, the maximum transmission of the TE-polarized wave and TM-polarized wave are different in the range of 1.2–1.8 THz, which can be used to distinguish different polarized incident waves. The corresponding transmissions of the TE-polarized wave demonstrate the opposite results with the different chemical potential of graphene, realizing the switching functions in the frequency band of 0.88–1.34 THz. When the operation frequency is above 2 THz, the multi-frequency rejection filter can be achieved. The proposed metamaterial structure can be applied in many advanced fields, including the fronthaul of terahertz communication system, electromagnetic stealth, radar, etc.