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A Tunable Dual-Band and Polarization-Insensitive Coherent Perfect Absorber Based on Double-Layers Graphene Hybrid Waveguide


A suspended monolayer graphene has only about 2.3% absorption rate in visible and infrared band, which limits its optoelectronic applications. To significantly increase graphene’s absorption efficiency, a tunable dual-band and polarization-insensitive coherent perfect absorber (CPA) is proposed in the mid-infrared regime, which contains the silicon array coupled in double-layers graphene waveguide. Based on the FDTD methods, dual-band perfect absorption peaks are achieved in 9611 nm and 9924 nm, respectively. Moreover, due to its center symmetric feature, the proposed absorber also demonstrates polarization-insensitive. Meanwhile, the coherent absorption peaks can be all-optically modulated by altering the relative phase between two reverse incident lights. Furthermore, by manipulating the Fermi energies of two graphene layers, two coherent absorption peaks can move over a wide spectrum range, and our designed CPA can also be changed from dual-band CPA to narrowband CPA. Thus, our results can find some potential applications in the field of developing nanophotonic devices with excellent performance working at the mid-infrared regime.


As a crucial issue for nanophotonics and optoelectronics, efficient light-matter interaction has widely caused concerns in recent years [1, 2], particularly in the atomically thin two-dimension (2D) materials. Many reports have been demonstrated, such as transition-metal dichalcogenides (TMDCs) [3, 4], graphene [5,6,7,8,9], hexagonal boron nitride [10], black phosphorus [11], and so on. As a prototypical 2D material, graphene can interact with light in a wide (ultraviolet to terahertz) wavelength range. However, due to its natural gapless and conical electronic band structure [12], the absorption efficiency of light in graphene is as low as about 2.3%. Fortunately, the optical bandgap of graphene can be opened up by doping or using the other special methods, which results in the excitation of surface plasmon polaritons (SPPs) in the terahertz and infrared bands [13]. Then, the absorption and confinement of light in graphene can be remarkably strengthened because of the excited SPPs, which can prolong the interaction time between graphene and light [14,15,16,17,18,19]. Therefore, graphene plasmonic devices have become an interesting and significant topic, and extensive researches have been demonstrated in various fields, such as absorbers [17, 18], optical filters [20], sensors [21], modulators [22], and photodetectors [23, 24].

More specifically, among these devices based on graphene, optical absorber takes an important role in the field of developing advanced optoelectronic devices, such as solar energy-trapping devices and emitters. Recently, due to the unique attributes of graphene, some absorbers based on graphene have been reported. Moreover, as mentioned above, most of these absorbers are focused on the terahertz and infrared regimes, because graphene with special processes can excite SPPs, leading to the strong light-graphene interactions in these wavelengths [3]. For instance, based on graphene, Luo et al. [25] proposed a tunable perfect absorber with ultra-narrowband, which can maintain satisfactory performances under broad-angle incidence. In Ref. [16], by embedding monolayer graphene to the metamaterials, Xiao et al. demonstrated that the EIT analog was realized in the terahertz regime, and its resonance intensity could be flexibly manipulated over a wide range. Jiang et al. [26] designed, fabricated, and investigated a broadband absorber based on patterned graphene in the terahertz regime, and the absorption above 90% is achieved from 1.54 to 2.23 THz. In order to manipulate the surface plasmon of graphene in an effective and feasible way, Xia et al. suggested that it could be realized by using a conductive sinusoidal grating with sub-wavelength size [19].

Importantly, coherent perfect absorber (CPA), which is another way to control and strengthen the optical absorption of graphene, has attracted great attention due to the all-optical modulation features [27, 28]. Depending on the interference effects and interplay of absorption, CPA provides a potential method to manipulate light with light without nonlinearity. Y. D. Chong et al. theoretically investigated the CPA with the scattering matrix [29]. Before long, two kinds of CPA were successively reported in the silicon slab [30] and planar metamaterial [31]. Recently, CPA has also been intensively studied in graphene-based devices. For example, combined with centrosymmetry metal-graphene nanostructure, Y. Ning et al. [32] investigated a tunable polarization-insensitive CPA and showed that the absorption could be flexibly and all-optically modulated by the Fermi energy of graphene and the relative phase between the incident lights. By trapping the guided-mode resonance in a subwavelength dielectric grating, X. Feng et al. [33] realized a tunable graphene-based CPA, which can be applied in a wide spectrum coverage from visible to infrared regimes. Y. C. Fan et al. [34] exploited graphene nanoribbon-based metasurface to CPA in the mid-infrared regime, and demonstrated that this CPA can be manipulated flexibly by changing the properties of graphene and structural parameters of the metasurface. However, the dual-band graphene-based CPA is also of great significance to the nanophotonics and optoelectronics devices, but seldom investigated in the mid-infrared regime. Furthermore, how to improve its adjustability is also a challenge facing the dual-band CPA.

In this paper, we design and study a tunable dual-band and polarization-insensitive CPA in the mid-infrared band, which contains a silicon array coupled in double-layers graphene waveguide. The physical mechanism of the designed CPA is analyzed by the scattering matrix. Meanwhile, the features of proposed CPA are demonstrated by the finite-difference time-domain (FDTD) simulations. When the incident light is illuminated into the silicon array, since the plasmonic resonances on the double continuous graphene films can be emerged due to the mechanism of guided-mode resonance, then the coupling effect between them results in the perfect dual-band absorption peaks, which are achieved in 9611 nm and 9924 nm, respectively. Moreover, due to its center symmetric feature, the proposed absorber also demonstrates polarization-insensitive. Furthermore, most of the reported graphene-based absorbers are manipulated by only changing the properties of graphene through an electrostatic field, magnetic field, or chemical doping, which are the causes of additional losses and also make the devices more complicated. For our proposed CPA, the coherent absorptions can be all-optically modulated by altering the relative phase between two reverse incident lights, which improves the absorber’s adjustability and does not increase the complexity of the structure. Meanwhile, by manipulating the Fermi energies of two graphene layers, two coherent absorption peaks can move over a wide spectrum range, and our designed CPA can also be changed from dual-band CPA to narrowband CPA. Therefore, our work provides a very promising way with convenience and sensitivity for potential applications include switches, all-optical logical devices, and coherent photodetectors.


As illustrated in Fig. 1, there are two continuous graphene films on the silica substrate, which are separated by a silica layer. Meanwhile, the silicon array is put on the top of upper graphene film. Here, the length (x-direction) and width (y-direction) of every silicon square in the array are both set as w = 80 nm, as shown in Fig. 1c. Meanwhile, both the periods of silicon squares in the x-direction and y-direction are p = 160 nm, and the thickness (z direction) of silicon square is h = 100 nm. Moreover, the thicknesses of the silica spacer and substrate are d1 = 75 nm and d2 = 150 nm, respectively. I1 and I2, as two coherent incident lights, are simultaneously irradiated on the proposed CPA from two contrary directions, as shown in Fig. 1a. The relationship between I1 and I2 is I2 = αI1 exp( + ikz), where α, φ, and z are the relative amplitude, phase difference, and phase reference point between I1 and I2, respectively. O1 and O2 are the emergent lights scattering from the bottom and top of proposed CPA. Furthermore, the thicknesses of two graphene films are both set as 0.34 nm in our simulations, and the conductivities of two graphene films are both computed within the local random phase approximation as follows [35]:

$$ \sigma \left(\omega \right)=\frac{ie^2{\kappa}_BT}{\pi {\mathrm{\hslash}}^2\left(\omega +i{\tau}^{-1}\right)}\left[\frac{E_f}{\kappa_BT}+2\ln \left({e}^{-\frac{E_f}{\kappa_BT}}+1\right)\right]+\frac{ie^2}{4\pi \mathrm{\hslash}}\ln \left[\frac{2{E}_f-\left(\omega +i{\tau}^{-1}\right)\mathrm{\hslash}}{2{E}_f+\left(\omega +i{\tau}^{-1}\right)\mathrm{\hslash}}\right] $$

where T = 300K is the room temperature and Ef is the Fermi energy. Meanwhile, the intrinsic relaxation time is described as \( \tau =\mu {E}_f/\mathrm{e}{\upsilon}_f^2 \), where υf is the Fermi velocity and μ = 10000cm2V−1s−1 is the carrier mobility. For our proposed structure, the Fermi energies of the upper and lower graphene films are assumed as Ef1 = 0.66eV and Ef2 = 0.31eV, respectively.

Fig. 1
figure 1

a Schematic diagram of the dual-band graphene-based perfect absorber. b Side view with dimensions specified. c Top view with dimensions specified

In the simulation, we utilize the 3D FDTD method for the numerical calculation. Meanwhile, periodic boundary conditions are applied along the x- and y-directions, and perfectly matched layer is applied along the z-direction including both the top and bottom of the proposed device. Moreover, we utilize the non-uniform mesh to compute the simulation results, where the minimum mesh size inside the graphene layer equals 0.1 nm and gradually increases outside the graphene film to cut down on the storage space and computing time.

Results and Discussion

Firstly, in order to clearly explain the physical mechanism, we investigate the absorption of proposed CPA under normal illumination of only one incident beam I1 in the z-direction. Since the graphene-based CPA is in the symmetry environment, the combined reflection and transmission coefficients can be expressed as r = η and t = 1 + η, respectively, where η is the self-consistent amplitude related to the graphene hybrid waveguide. Thus, the absorption is derived as A = 1 − |r|2 − |t|2 =  − 2η2 − 2η. The condition of maximum absorption is ∂A/∂η = 0 (∂A2/∂η2 is real and negative) and we get \( \eta =-\frac{1}{2} \). Then, the limit to maximum absorption is Amax = 0.5. In our simulation, when only one incident beam I1 vertically illuminates on the proposed absorber, due to the plasmonic resonances on the double graphene films, which are emerged by incident light through the silicon array for the mechanism of guided-mode resonance, then the coupling effect between the double graphene films leads to the dual-band absorption peaks, as demonstrated in Fig. 2. However, both two absorption peaks are less than 0.5, which accord with the absorption limit.

Fig. 2
figure 2

The reflection (R), transmission (T), and absorption (A) spectra of the proposed graphene-based absorber with Fermi energies Ef1 = 0.66 eV and Ef2 = 0.31 eV under the illumination of only one incident beam I1 in the z direction

Then, when I1 and I2 vertically incident on the proposed structure from opposite sides, the schematic diagram is shown in Fig. 1a. Meanwhile, O1 and O2 can also be assumed as the intensities of emergent lights from the bottom and top of the proposed CPA. The relationship between the incident lights and emergent lights is demonstrated by the scattering matrix:

$$ \left[\begin{array}{c}{O}_2\\ {}{O}_1\end{array}\right]=\left[\begin{array}{cc}{r}_{11}& {t}_{12}\\ {}{t}_{21}& {r}_{22}\end{array}\right]\left[\begin{array}{c}{I}_1\\ {}{I}_2\end{array}\right] $$

When the incoherent absorption limit is satisfied (i.e., r11 = r22 =  − 0.5 and t12 = t21 = 0.5), by considering the relationship I2 = αI1 exp( + ikz) with z = 0, the coherent absorption Aco of the proposed graphene-based CPA is express as [36]:

$$ {A}_{\mathrm{co}}=1-\frac{{\left|{O}_1\right|}^2+{\left|{O}_2\right|}^2}{{\left|{I}_1\right|}^2+{\left|{I}_2\right|}^2}=1-\frac{1+{\alpha}^2-2\alpha \cos \left(\varphi \right)}{2\left(1+{\alpha}^2\right)} $$

Thus, according to Eq. (3), Aco can be manipulated by changing α and φ. In particular, if α = 1, Aco can be tuned from the minimum Aco − min = 0 to the maximum Aco − max = 1 when φ varies from (2N + 1)π to 2.

As illustrated in Fig. 3, when two incident lights with φ = 0 and α = 1 are coherent illuminated on the proposed structure, dual-band perfect absorption peaks can be achieved in λ1 = 9611 nm and λ2 = 9924 nm, respectively. Moreover, compared with the absorption under the illumination of only one incident beam, the absorption of the proposed graphene-based CPA has been significantly enhanced. It is worth noting that due to its center symmetric feature, the proposed CPA also demonstrates polarization-insensitive. As shown in Fig. 3, whether the incident lights with p or s polarization, the absorption spectrum remains the same.

Fig. 3
figure 3

The absorption spectra of the proposed graphene-based absorber under the illumination of only one incident beam (red curve), and under coherent illumination with p polarization (blue curve) and s polarization (black curve)

To clearly demonstrate the features of proposed CPA, we illustrate the magnetic fields around the double-layers graphene waveguide at the wavelengths of absorption peaks. As described in Fig. 4a, b, the magnetic fields around two graphene layers are both gathered and trapped at the wavelengths of absorption peaks. However, for the upper graphene film, the magnetic fields are mainly confined between the silicon squares and the upper graphene film, which correspond to the localized plasmon mode. Moreover, once another graphene film is added below the upper graphene film, light energies will transfer from the upper layer to the lower one due to the guided-mode resonance. Then, the coupling effect between the upper graphene layer and the lower one enhances the optical fields and concentrates the light energies in the proposed structure, which leads to the dual-band absorption peaks, as shown in Fig. 3. On the other hand, at the wavelength of 9000 nm, there are few strengthened optical fields surrounding two graphene films, because it is far away from resonance wavelengths, as demonstrated in Fig. 4c.

Fig. 4
figure 4

Contour profiles of normalized magnetic fields of the proposed graphene-based CPA (a) at λ1 = 9611 nm, (b) λ2 = 9924 nm, and (c) λ3 = 9000 nm

Next, for the sake of displaying all-optical modulation characteristics, we demonstrate the coherent absorption of proposed absorber with different phase differences φ, as illustrated in Fig. 5. Meanwhile, the relative amplitude α of coherent incident lights is set as 1, and the other structural parameters are kept as the same as that in Fig. 1. As depicted in Fig. 5a, b, by increasing φ from 0 to π, two absorption peaks at 9611 nm and 9924 nm decrease continuously from 0.982 and 0.993 to almost 0, respectively. Thus, the modulation contrast can be as high as 34.8 dB and 35.2 dB at the two coherent absorption peaks with different φ, which shows a significant all-optical modulation property.

Fig. 5
figure 5

The absorption of proposed CPA with different phase difference at the peaks of a λ1 = 9611 nm and b λ2 = 9924 nm, respectively

In the following, for our four layers (silicon array-graphene waveguide/silica layer/graphene film/silica substrate) system, combined with continuous boundary conditions and the Maxwell equations, the dispersion relation can be expressed as [37]:

$$ \exp \left(-2{k}_2{d}_1\right)=\frac{1+\frac{\varepsilon_2{k}_1}{\varepsilon_1{k}_2}}{1-\frac{\varepsilon_2{k}_1}{\varepsilon_1{k}_2}}\bullet \frac{\left(1+\frac{\varepsilon_2{k}_3}{\varepsilon_3{k}_2}\right)\left(1+\frac{\varepsilon_3{k}_4}{\varepsilon_4{k}_3}\right)+\left(1-\frac{\varepsilon_2{k}_3}{\varepsilon_3{k}_2}\right)\left(1-\frac{\varepsilon_3{k}_4}{\varepsilon_4{k}_3}\right)\exp \left(-2{k}_3{d}_g\right)}{\left(1-\frac{\varepsilon_2{k}_3}{\varepsilon_3{k}_2}\right)\left(1+\frac{\varepsilon_3{k}_4}{\varepsilon_4{k}_3}\right)+\left(1+\frac{\varepsilon_2{k}_3}{\varepsilon_3{k}_2}\right)\left(1-\frac{\varepsilon_3{k}_4}{\varepsilon_4{k}_3}\right)\exp \left(-2{k}_3{d}_g\right)} $$

where, εi and ki (i = 1, 2, 3, 4) are the permittivities and wave vectors of the silicon array-graphene waveguide (i = 1), silica layer (i = 2), graphene film (i = 3), and silica substrate (i = 4), respectively. dg is the thickness of graphene. Thus, by properly manipulating the Fermi energies of two graphene films, the features of plasmonic modes sustained by two graphene films could be significantly and independently controlled. As seen in Fig. 6a, b, the absorption spectra of the proposed CPA can be flexibly and separately manipulated by altering the Fermi energies of lower-layer or upper-layer graphene film. When the Fermi energy Ef1 of upper-layer graphene remains unchanged and the Fermi energy Ef2 of lower-layer graphene decreases from 0.31 to 0.27 eV, the absorption peak at λ1 red-shifts and keeps the value almost unchanged, while the absorption peak at λ2 reduces rapidly and even disappears under Ef2 = 0.27 eV, as shown in Fig. 6a. On the contrary, when Ef2 increases from 0.31 to 0.37 eV, the absorption peak at λ1 reduces rapidly and almost disappears under Ef2 = 0.37 eV, while the absorption peak at λ2 blue-shifts and keeps the value almost unchanged. Thus, the dual-band proposed perfect absorber can be changed to narrow-band perfect absorber by separately altering the Ef2. On the other hand, when Ef2 remains unchanged and Ef1 increases from 0.62 to 0.72 eV, both two absorption peaks blue-shifts and keeps their values almost unchanged over a wide wavelength range, which demonstrates a significantly tunable characteristic. Compared with the other absorbers based on the discrete graphene patterns, it is worth noting that two graphene films of the proposed CPA are in the continuous form, which is more convenient to get excellent tunability.

Fig. 6
figure 6

Absorption spectra as a function of the wavelength and Fermi levels of a lower-layer graphene and b upper-layer graphene. The other structural parameters are the same as Fig. 1

In addition, we investigate the influences of different structure parameters on the optical absorption of proposed CPA, as shown in Fig. 7. Since each silicon square performances as a Fabry-Perot resonator for the localized plasmon mode, and the resonant wavelength is remarkably sensitive to the width of silicon squares. Thus, as shown in Fig. 7a, when the w is increased, dual-band absorption peaks are both red-shifted due to the increment of effective resonance wavelength of localized plasmon mode. Moreover, the filling factor will increase with w, which further reinforces the intensity of field enhancement and concentration between neighboring silicon square and inside graphene. Thus, the absorption efficiency will firstly increase with w. However, with the continuous increment of filling factor, too many areas of graphene will be covered by silicon squares. As a result, the absorption efficiency will subsequently decrease with the increment of w. Then, as shown in Fig. 7b, the absorption peaks will also be noticeably red-shifted with the increment of p, because the resonant wavelength of localized plasmon mode becomes larger. Furthermore, it is noted that the resonant frequency of the plasmonic mode supported by the lower-layer graphene strongly depends on the separation distance d1. As shown in Fig. 7c, when d1 is increased, the nearfield coupling strength between the upper- and lower-layer resonance modes will become more and more weak, which lead the dual-band absorption peaks eventually to degenerate into one peak. Meanwhile, we also investigate the absorption of proposed CPA with different dielectric array. As shown in Fig. 7d, the performances of dual-band CPA with whether the TiO2 array (nT = 2.9) or the GaSb array (nG = 3.8) is not better than the one with silicon array. Moreover, it is worth noting that the wavelengths of absorption peaks are red-shifted with the increment of the refractive index of the dielectric array.

Fig. 7
figure 7

Light absorption of proposed CPA with different a p, b w, c d1, and d different dielectric array, respectively. The other parameters are the same as Fig. 2


As mentioned before, most reported graphene-based perfect absorbers are polarization-sensitive and focused on the narrowband or broadband perfect absorbers, dual-band graphene-based perfect absorbers are seldom investigated in the mid-infrared regime. In this paper, we have designed a tunable dual-band and polarization-insensitive CPA in the mid-infrared regime, and the corresponding absorption features are discussed by using the scattering matrix and FDTD simulation, which illustrate that dual-band perfect absorption peaks are achieved in 9611 nm and 9924 nm, respectively. Moreover, due to its center symmetric feature, the proposed CPA also exhibits polarization-insensitive. Meanwhile, the coherent absorption peaks can be all-optically modulated by altering the relative phase between two reverse incident lights. Furthermore, by manipulating the Fermi energies of two graphene layers, two coherent absorption peaks can move over a wide spectrum range, and our designed CPA can also be changed from dual-band CPA to narrowband CPA. On the other hand, for the proposed CPA, subwavelength metamaterials based on silicon squares can be integrated for the current CMOS technology, and chemical vapor deposition (CVD) grown graphene can be transferred over the silica layer using standard transfer techniques [38]. Moreover, compared with the devices based on patterned graphene, our structure keeps graphene in the continuous form, which has the benefit of preserving the high mobility of graphene and simplifies the fabrication processes as well as the doping configuration. In recent years, some research groups have tried to design some graphene-based devices in an experiment based on the above methods [39,40,41]. Therefore, we believe it is possible to fabricate our proposed structure with similar processing, and our proposed graphene-based CPA can find some potential applications in the field of developing nanophotonic devices at the mid-infrared regime.

Availability of Data and Materials

All data generated or analyzed during this study are included in this published article.





Coherent perfect absorber


Finite-difference time-domain


Indium tin oxide


Surface plasmon polaritons


Transition-metal dichalcogenides


  1. Geim AK, Grigorieva IV (2013) Van der Waals heterostructures. Nature 499:419–425

    CAS  Article  Google Scholar 

  2. Qin M, Wang LL, Zhai X, Chen DC, Xia SX (2017) Generating and manipulating high quality factors of fano resonance in nanoring resonator by stacking a half nanoring. Nanoscale Res Lett 12:578

    Article  Google Scholar 

  3. Luo X, Zhai X, Wang LL, Lin Q (2018) Enhanced dual-band absorption of molybdenum disulfide using plasmonic perfect absorber. Opt Express 26:11658–11666

    CAS  Article  Google Scholar 

  4. Luo X, Liu ZM, Cheng ZQ, Liu JP, Lin Q, Wang LL (2018) Polarization-insensitive and wide-angle broadband absorption enhancement of molybdenum disulfide in the visible regime. Opt Express 26:33918–33929

    CAS  Article  Google Scholar 

  5. Yu P, Besteiro LV, Huang YJ, Wu J, Fu L, Tan HH, Jagadish C, Wiederrecht GP, Govorov AO, Wang ZM (2019) Broadband metamaterial absorbers. Adv Opt Mater 7:1800995

    Article  CAS  Google Scholar 

  6. Lin H, Sturmberg BCP, Lin KT, Yang YY, Zheng XR, Chong TK, Sterke CM, Jia BH (2019) A 90-nm-thick graphene metamaterial for strong and extremely broadband absorption of unpolarized light. Nat Photonics 13:270–276

    CAS  Article  Google Scholar 

  7. Xiao D, Liu Q, Lei L, Sun YL, Ouyang ZB, Tao KY (2019) Coupled resonance enhanced modulation for a graphene-loaded metamaterial absorber. Nanoscale Res Lett 14:32

    Article  CAS  Google Scholar 

  8. Yu P, Besteiro LV, WuJ HYJ, Wang YQ, Govorov AO, Wang ZM (2019) Metamaterial perfect absorber with unabated size-independent absorption. Opt Express 26:20471–20480

    Article  Google Scholar 

  9. Vakil A, Engheta N (2011) Transformation optics using graphene. Science 332:1291–1294

    CAS  Article  Google Scholar 

  10. Wu J, Jiang L, Guo J, Dai X, Xiang Y, Wen S (2016) Turnable perfect absorption at infrared frequencies by a graphene-hBN hyper crystal. Opt Express 24:17103–17114

    CAS  Article  Google Scholar 

  11. Lu H, Gong YK, Mao D, Gan XT, Zhao JL (2017) Strong plasmonic confinement and optical force in phosphorene pairs. Opt Express 25:5255–5263

    CAS  Article  Google Scholar 

  12. Bonaccorso F, Sun Z, Hasan T, Ferrari AC (2010) Graphene photonics and optoelectronics. Nature Photon 4:611–622

    CAS  Article  Google Scholar 

  13. Xiao SY, Liu TT, Zhou CB, Jiang XY, Cheng L, Liu YB, Li Z (2019) Strong interaction between graphene and localized hot spots in all-dielectric metasurfaces. J Phys D Appl Phys 52:385102

    CAS  Article  Google Scholar 

  14. Gan X, Mak KF, Gao Y, You Y, Hatami F, Hone J, Heinz TF, Englund D (2012) Strong enhancement of light-matter interaction in graphene coupled to a photonic crystal. Nano Lett 12:5626

    CAS  Article  Google Scholar 

  15. Xiao S, Wang T, Liu Y, Xu C, Han X, Yan X (2016) Tunable light trapping and absorption enhancement with graphene ring arrays. Phys Chem Chem Phys 18:26661–26669

    CAS  Article  Google Scholar 

  16. Xiao S, Wang T, Liu T, Yan X, Li Z, Xu C (2018) Active modulation of electromagnetically induced transparency analogue in terahertz hybrid metal-graphene metamaterials. Carbon 126:271–278

    CAS  Article  Google Scholar 

  17. Li HJ, Wang LL, Zhai X (2016) Tunable graphene-based mid-infrared plasmonic wide-angle narrowband perfect absorber. Sci Rep 6:36651

    CAS  Article  Google Scholar 

  18. Zhang YP, Li TT, Chen Q, Zhang HY, Hara JFO, Abele E, Taylor AJ, Chen HT, Azad AK (2015) Independently tunable dualband perfect absorber based on graphene at mid-infrared frequencies. Sci Rep 5:18463

    CAS  Article  Google Scholar 

  19. Xia SX, Zhai X, Huang Y, Liu JQ, Wang LL, Wen SC (2017) Graphene surface plasmons with dielectric metasurfaces. J Lightw Technol 35:4553–4558

    CAS  Article  Google Scholar 

  20. Luo X, Zhai X, Wang LL, Lin Q (2015) Narrow-band plasmonic filter based on graphene waveguide with asymmetrical structure. Plasmonics 10:1427–1431

    CAS  Article  Google Scholar 

  21. Echtermeyer TJ, Britnell L, Jasnos PK, Lombardo A, Gorbachev RV, Grigorenko AN, Geim AK, Ferrari AC, Novoselov KS (2011) Strong plasmonic enhancement of photovoltage in graphene. Nat Commun 2:458

    CAS  Article  Google Scholar 

  22. Liu M, Yin XB, Ulin-Avila E, Geng BS, Zentgraf T, Ju L, Wang F, Zhang X (2011) A graphene-based broadband optical modulator. Nature 474:64–67

    CAS  Article  Google Scholar 

  23. Mueller T, Xia F, Avouris P (2010) Graphene photodetectors for high-speed optical communications. Nature Photon 4:297–301

    CAS  Article  Google Scholar 

  24. Yu R, Pruneri V, Abajo FJGD (2016) Active modulation of visible light with graphene-loaded ultrathin metal plasmonic antennas. Sci Rep 6:32144

    CAS  Article  Google Scholar 

  25. Luo X, Liu ZM, Wang LL, Liu JP, Lin Q (2018) Tunable ultra-narrowband and wide-angle graphene-based perfect absorber in the optical communication region. Appl Phys Exp 11:105102

    Article  Google Scholar 

  26. Jiang YN, Zhang HD, Wang J, Gao CN, Wang J, Cao WP (2017) Design and performance of a terahertz absorber based on patterned graphene. Opt Lett 43:4296–4299

    Article  Google Scholar 

  27. Rothenberg JM, Chen CP, Ackert JJ, Dadap JI, Knights AP, Bergman K, Osgood RM, Grote RR (2016) Experimental demonstration of coherent perfect absorption in a silicon photonic racetrack resonator. Opt Lett 41:2537–2540

    CAS  Article  Google Scholar 

  28. Dutta-Gupta S, Martin OJF, Gupta SD, Agarwal GS (2012) Controllable coherent perfect absorption in a composite film. Opt Express 20:1330–1336

    Article  Google Scholar 

  29. Chong YD, Ge L, Cao H, Stone AD (2010) Coherent perfect absorbers: time-reversed lasers. Phys Rev Lett 105:053901

    CAS  Article  Google Scholar 

  30. Wan W, Chong Y, Ge L, Noh H, Stone AD, Cao H (2011) Time-reversed lasing and interferometric control of absorption. Science 331:889–892

    CAS  Article  Google Scholar 

  31. Zhang J, MacDonald KF, Zheludev NI (2012) Controlling light-with-light without nonlinearity. Light Sci Appl 1:e18

    Article  CAS  Google Scholar 

  32. Ning Y, Dong Z, Si J, Deng X (2017) Tunable polarization-independent coherent perfect absorber based on a metal-graphene nanostructure. Opt Express 25:32467–32474

    CAS  Article  Google Scholar 

  33. Feng X, Zou JL, Xu W, Zhu ZH, Yuan XD, Zhang JF, Qin SQ (2018) Coherent perfect absorption and asymmetric interferometric light-light control in graphene with resonant dielectric nanostructures. Opt Express 26:29183–29191

    CAS  Article  Google Scholar 

  34. Fan YC, Liu Z, Zhang FL, Zhao Q, Wei ZY, Fu QH, Li JJ, Gu CZ, Li HQ (2015) Tunable mid-infrared coherent perfect absorption in a graphene meta-surface. Sci Rep 5:13956

    CAS  Article  Google Scholar 

  35. Hanson GW (2008) Dyadic Green’s functions and guided surface waves for surface conductivity model of graphene. J Appl Phys 103:064302

    Article  CAS  Google Scholar 

  36. Zhang J, Guo C, Liu K, Zhu Z, Ye W, Yuan X, Qin S (2014) Coherent perfect absorption and transparency in a nanostructured graphene film. Opt Express 22:12524–12532

    Article  CAS  Google Scholar 

  37. Xu HJ, Lu WB, Zhu W, Dong ZG, Cui TJ (2012) Efficient manipulation of surface plasmon polariton waves in graphene. Appl Phys Lett 100:243110

    Article  CAS  Google Scholar 

  38. Suk JW, Kitt A, Magnuson CW, Hao Y, Ahmed S, An J, Swan AK, Goldberg BB, Ruoff RS (2011) Transfer of CVD-grown monolayer graphene onto arbitrary substrates. ACS Nano 5:6916–6924

    CAS  Article  Google Scholar 

  39. Liu YH, Chadha A, Zhao D, Piper JR, Jia YC, Shuai YC, Menon L, Yang HJ, Ma ZQ, Fan SH, Xia FN, Zhou WD (2014) Approaching total absorption at near infrared in a large area monolayer graphene by critical coupling. Appl Phys Lett 105:181105

    Article  CAS  Google Scholar 

  40. Zhao WY, Leng XD, Jiang YY (2015) Fano resonance in all-dielectric binary nanodisk array realizing optical filter with efficient linewidth tuning. Opt Express 23:6858–6866

    CAS  Article  Google Scholar 

  41. Sun F, Xia L, Nie C, Shen J, Zou Y, Cheng G, Wu H, Zhang Y, Wei D, Yin S, Du C (2018) The all-optical modulator in dielectric-loaded waveguide with graphene-silicon heterojunction structure. Nanotechnology 29:135201

    Article  CAS  Google Scholar 

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This work was supported by the National Natural Science Foundation of China (Grant nos. 61775055, 61505052, 61764005, and 11804093); Natural Science Foundation of Jiangxi Province (nos. 20181BAB201013 and 20192BAB212003).

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XL, ZQC, XZ, and ZML designed the study and analyzed the data. SQL, JPL, LLW, LQ, and YHZ helped in data analysis and manuscript modification. All the authors have read and approved the final manuscript.

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Correspondence to Zi-Qiang Cheng or Zhi-Min Liu.

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Luo, X., Cheng, ZQ., Zhai, X. et al. A Tunable Dual-Band and Polarization-Insensitive Coherent Perfect Absorber Based on Double-Layers Graphene Hybrid Waveguide. Nanoscale Res Lett 14, 337 (2019).

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  • Graphene
  • Absorption
  • Surface plasmons