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Dynamically Tunable Plasmon-Induced Transparency in On-chip Graphene-Based Asymmetrical Nanocavity-Coupled Waveguide System
Nanoscale Research Lettersvolume 12, Article number: 374 (2017)
A graphene-based on-chip plasmonic nanostructure composed of a plasmonic bus waveguide side-coupled with a U-shaped and a rectangular nanocavities has been proposed and modeled by using the finite element method in this paper. The dynamic tunability of the plasmon-induced transparency (PIT) windows has been investigated. The results reveal that the PIT effects can be tuned via modifying the chemical potential of the nanocavities and plasmonic bus waveguide or by varying the geometrical parameters including the location and width of the rectangular nanocavity. Further, the proposed plasmonic nanostructure can be used as a plasmonic refractive index sensor with a sensing sensibility of 333.3 nm/refractive index unit (RIU) at the the PIT transmission peak. Slow light effect is also realized in the PIT system. The proposed nanostructure may pave a new way towards the realization of graphene-based on-chip integrated nanophotonic devices.
Plasmon-induced transparency (PIT), which is a novel phenomenon analogous to electromagnetically induced transparency (EIT) effect generating a sharp transparency window within a broad absorption spectrum , has attracted great attention due to its potential applications in a wide range of fields, such as slow light [2, 3], optical switching , light storage , and high-sensitivity sensing [6, 7]. The PIT-based devices can be realized with ultra-compact footprint because of the large local field enhancement ability and overcoming of classical diffraction limit of light provided by the surface plasmon polaritons (SPPs) [8, 9]. A variety of designs have been proposed to achieve PIT effect in plasmonic nanostructures including coupled resonator systems [10,11,12,13], photonic crystal structures [14, 15], and metamaterial structures [16, 17]. However, most of these structures displaying PIT effect are barely tunable unless changing the geometrical parameters of the structures, which in a large extent limit the active control of PIT windows and degrade the quality.
Graphene, a monolayer of carbon atoms arranged in a two-dimensional (2D) honeycomb lattice , shows great potential for developing highly efficient optoelectronic devices due to its exceptional electrical and optical properties including the ability of extreme confinement [19,20,21], dynamic tunability, and relatively low damping losses [22, 23]. Particularly, the surface conductivity of graphene can be dynamically tuned by chemical potential via external gate voltage or chemical doping [24, 25], which makes graphene to be a promising candidate for designing tunable PIT while the geometrical parameters are fixed. Because of these extraordinary features compared to those of conventional noble metals, a wide range of researches have been done to realize graphene-based PIT, such as PIT phenomena in graphene ring resonator-coupled graphene waveguide [26, 27] and PIT effects in a graphene-based nanoribbon waveguide coupled with graphene rectangular resonator structure [28, 29]. Sun et al. studied the periodically patterned graphene double-layer structure separated by a dielectric layer in the terahertz frequency range, where the multispectral PIT responses have been achieved . Furthermore, tunable PIT effects are realized in the periodically combined graphene nanostrips and analytically described with the coupled Lorentz oscillator model [31, 32]. However, most of the previous works were concerned about graphene resonators, coupled to a monolayer graphene or a graphene nanoribbon waveguide system, and graphene nanostrip systems with normal incident light. There were very few or even no studies about plasmonically induced transparency phenomenon in a graphene sheet with locally variant chemical potentials. Further, compared with normal incident light, in plane propagation has overwhelming advantages for on-chip integration.
Motivated by the above fundamental studies, in this paper, we propose a graphene-based plasmonic nanostructure composed of a plasmonic bus waveguide side-coupled to a U-shaped nanocavity and a rectangular nanocavity on the same graphene monolayer. The commercial software COMSOL Multiphysics based on finite element method (FEM) is utilized to explore the transmission and electromagnetic responses of our designs. Simulation results reveal that the PIT phenomenon is observed in our proposed plasmonic nanostructure. Further, the PIT window can be effectively tuned by varying the chemical potentials of the nanocavities and plasmonic bus waveguide. Also, a coupled mode theory (CMT) is introduced to explain the transmission features of the PIT phenomenon. At last, a plasmonic refractive index sensor based on the proposed plasmonic nanostructure is studied. The sensing sensitivity of 333.3 nm/refractive index unit (RIU) is achieved at the PIT transmission peak. Also, the slow light effect with group delay over 1 ps is realized. This proposed novel plasmonic nanostructure may offer a new way to realize graphene-based on-chip high-density plasmonic device integration on a graphene monolayer.
For the sake of simplicity, the proposed structure is modeled by a suspended graphene monolayer with local variation of chemical potential to form the corresponding bus waveguide and the nanoresonators. Figure 1a shows the schematic configuration and geometric parameters of a U-shaped nanocavity directly coupled to a plasmonic bus waveguide. The U-shaped nanocavity coupled waveguide with a chemical potential of μ c2 is surrounded by the same sheet of graphene with chemical potential of μ c1. The width of the plasmonic bus waveguide d is 20 nm. The width and height of the U-shaped nanocavity are W U = 150 nm and L U = 120 nm respectively. Exact theoretical modeling of such a structure requires a three-dimensional (3D) computation, which is extremely time- and memory-consuming. To solve this problem, the effective index method has been used by many publications [33,34,35], and the refractive index of the structure is replaced by the effective index of guided modes, which is defined by the ratio between the propagation constant and the wave number in the free space. In our structure, the graphene sheet is treated as an ultrathin film which is characterized by effective index defined as n eff = β/k 0, where k 0 = 2π/λ is the wave number in free space. The propagation constant β of the guided SPP mode supported by monolayer graphene is written as [36, 37]
where μ 0 and ε 0 represent the permeability and permittivity of vacuum, respectively, and μ r and ε r represent the relative permeability and relative permittivity respectively. The surface conductivity of graphene σ g composed of the interband electron transitions σ inter and the intraband electron-photon scattering σ intra is given by the Kubo formula [38, 39]
where μ c is the chemical potential of graphene, ω is the angular frequency of the plasmon, ћ is the reduced Planck’s constant, e is the electron charge, k B is the Boltzmann’s constant, T is the temperature, ℏ = h/2π is the reduced Planck’s constant, and τ is the electron momentum relaxation time. Specifically, the chemical potential of graphene can be tuned via chemical doping or electrical gating [25, 26]. Mikhailov et al. have experimentally shown that the carrier density in a graphene sheet as high as 1014 cm−2 had been achieved, which led to a chemical potential of 1–2 eV at a temperature below 250 K . Furthermore, it has been demonstrated that high-quality suspended graphene with direct current mobility as high as 105 cm2V−1s−1 can be obtained, which corresponds to τ > 1.5 ps . In this paper, both the relaxation time and chemical potential we set are conservative enough to ensure the reliability of our numerical study.
Results and Discussion
As the SPP wave passes through the side-coupled U-shaped nanocavity shown in Fig. 1a, the energy is coupled into the nanocavity. A deep transmission valley is obtained at the resonance wavelength due to the destructive interference between the incident wave and escaped power from the nanocavity [12, 13]. Figure 1b plots the transmission spectrum of a U-shaped nanocavity directly coupled to a plasmonic bus waveguide with τ = 1 ps, μ c1 = 0.3 eV, and μ c2 = 0.9 eV. A pronounced dip with transmittance less than 0.1 is achieved at the resonance wavelength of 2437 nm. The inset in Fig. 1b shows the corresponding electric field distribution at the resonance wavelength, where it can be seen that almost no SPPs propagate through the plasmonic waveguide. Figure 2a displays the transmittance spectra with varied relaxation time τ = 0.6, 0.8, and 1 ps, where it can be seen that a higher transmission contrast is achieved when the relaxation time increases. This is attributed to the reduction of the Ohmic absorption of the plasmons when the relaxation time of electron momentum increases . The calculated transmittance of a U-shaped nanocavity-coupled waveguide system for different chemical potentials μ c2 is presented in Fig. 2b. The relaxation time τ and chemical potential μ c1 are constantly kept as 1 ps and 0.3 eV respectively. One can see that the locations of dips are dynamically tuned via varied chemical potential of the nanocavity and bus waveguide. The central wavelengths of the dips are 2455, 2445, and 2437 nm with μ c2 = 0.89, 0.895, and 0.9 eV respectively.
where 1/τ i and 1/τ e represent the decay rate of the intrinsic loss in the nanocavity and the power escaping through the plasmonic bus waveguide respectively. Obviously, the minimum transmittance T min = (1/τ i)2/(1/τ i + 1/τ e)2 can be achieved when the frequency of incident light ω is equal to the resonance frequency ω 0. As the 1/τ e is much more than 1/τ i , a transmission dip nearly zero can be obtained, which agrees well with the simulation results.
In order to obtain PIT effects, we add a rectangular nanocavity based on the plasmonic nanostructure shown in Fig. 1. A graphene-based plasmonic nanostructure composed of a plasmonic bus waveguide side-coupled to U-shaped and rectangular nanocavities is schematically shown in Fig. 3a. There exists strong coupling between the two nanocavities when they are connected via the plasmonic bus waveguide. The destructive interference between two resonant excitation pathways related to the U-shaped and rectangular nanocavities generates the PIT phenomenon [10, 11]. As shown in Fig. 3b, a sharp transmission peak (increased from 0.06 to 0.44) appeared in the transmission forbidden band shown in Fig. 1b implying the formation of the PIT window. The central wavelength of the PIT window is 2437 nm which is exactly the location of the central wavelength of the transmission dip shown in Fig. 1b. The broad resonant of the U-shaped nanocavity is split into two resonant modes: one is blueshifted while the other is redshifted [12, 13]. Figure 3c–e displays the electric field distributions of resonant modes at 2408, 2437, and 2457 nm respectively. We can see that the electric field distribution in the nanocavities is in-phase with the electric field distribution in plasmonic bus waveguides at 2437 nm, which means that the incident light and the light escaping into the plasmonic bus waveguide from the nanocavities encounter a coherent enhancement. Furthermore, the electric field distributions reveal that there is anti-phase between the nanocavities and plasmonic bus waveguide at 2408 and 2457 nm, i.e., the conditions of destructive resonance have been met which results in the inhibition of the transmission waves .
We calculate the spectral transmittance for the U-shaped and rectangular nanocavity-coupled plasmonic bus waveguide system with varied relaxation time τ = 0.6, 0.8, and 1 ps, and the results are shown in Fig. 4a. One can see that the transmission contrast increases with the increasing of relaxation time. Moreover, the dynamic tunability of the PIT window is shown in Fig. 4b. The chemical potential μ c1 is constantly kept as 0.3 eV, while μ c2 is 0.89, 0.895, and 0.9 eV. As the chemical potential μ c2 increases, the transmission peak (at the wavelengths of 2452, 2445, and 2437 nm) in the PIT window is obviously blueshifted. As a result, the dynamically tunable PIT effect is realized in our proposed nanostructure by modifying the chemical potential of the nanocavities and plasmonic bus waveguide.
To investigate how the geometrical parameters influence the PIT phenomenon, we modified the location of the rectangular nanocavity. Figure 5a shows the spectral transmittance of the U-shaped and rectangular nanocavity-coupled plasmonic bus waveguide system, where it is seen that the transmission peak got higher (increased from 0.44 to 0.52) and the PIT window becomes broader with L 2 increasing for a certain range, which is attributed to the intensification of the coupling strength between the two nanocavities [11, 28]. Also, we find that the decreasing of the width of rectangular nanocavity can lead to a higher transmission peak (increased from 0.44 to 0.48) as shown in Fig. 5b. This offers another option to tune the PIT window. The quality factor (Q-factor) of the PIT windows is defined as λ 0 /∆λ, where λ 0 and ∆λ are transmission peak wavelength and full width at half maximum (FWHM). In our proposed plasmonic nanostructure, a FWHM of less than 30 nm and Q-factor of around 80 is obtained, which is much narrower and higher than the counterparts of graphene-based PIT proposed in the aforementioned references [28, 29].
where γ and β stand for the coupling coefficient between the two nanocavities and the coupling coefficient between the nanocavities and plasmonic bus waveguide respectively. We can find that the PIT window can be obtained when the resonant frequencies of the U-shaped nanocavity ω U and the rectangular nanocavity ω r are approximately equivalent. And the corresponding transmission peak is |( γ + 1)/(β + γ + 1)|2.
Based on the structure shown in Fig. 3a, we construct the refractive index sensor, which is realized by modifying the relative permittivity in Eq. 1. Figure 6a illustrates the spectral transmittance with different refractive index n, which refers to the refractive index of the undersensing material. One can see that the peak/dip1/dip2 wavelengths shift from 2437.3 to 2457.3 nm/2410.3 to 2432.4 nm/2457.3 to 2474.9 nm when the refractive index n varies from 1 to 1.06. As the refractive index n increases, both the transmission peak and dips exhibit a redshift. The sensing sensitivity of refractive index sensor, defined as the shift in the peak/dip1/dip2 wavelength per unit variations of the refractive index dλ/dn is 333.3, 368.3, and 293.3 nm/RIU respectively. Figure 6b shows the peaks and dips of the spectral transmittance with refractive index n varying from 1 to 1.19, where we can see the approximately linear relationship of the peak/dip wavelengths versus the refractive index n.
It is well known that the PIT phenomenon is accompanied by the slow light effect caused by the sharp dispersion [13, 29]. The slow light effect can be characterized by the group delay expressed as τ g = ∂φ(ω)/∂ ω where φ(ω) is the effective phase shift of the transmission spectrum. In Fig. 7, we plot the group delays within the PIT window at different chemical potential μ c2. In the vicinity of the PIT transmission peak, it offers large positive group delays indicating the slow light effect. The peak wavelengths of the PIT system at μ c2 = 0.89, 0.895, and 0.9 eV are 2449.7, 2442.3, and 2434.7 nm, respectively, and the corresponding group delays are 0.99, 1.1, and 1.02 ps respectively. Thus, the slow light effect is effectively tuned by modifying the chemical potential of the nanocavities and the plasmonic bus waveguide. It should also been pointed out that this is a proof-of-concept article. In reality, the proposed structure should lie on the substrate, where the refractive index is larger than the air, and the frequency response would shift accordingly. Also, the confinement of the plasmon is higher, accompanying by the increasing of the loss, which results in the reduction of the peak value of the transparence window in the transmission spectrum. However, the principle is identical to the suspended case.
In conclusion, dynamically tunable PIT effects in graphene-based plasmonic nanostructure composed of a plasmonic bus waveguide side-coupled to U-shaped and rectangular nanocavities have been proposed and modeled by using finite element method. The dynamic tunability of the PIT windows is obtained by modifying the chemical potential of the nanocavities and plasmonic bus waveguide. Furthermore, the PIT window can be tuned dynamically via adjusting the geometrical parameters of the nanostructure, such as the location and width of the rectangular nanocavity. Compared to the conventional ring resonators [24, 25], our proposed asymmetric U-shaped and rectangular resonators offer stronger coupling strength between the resonators and the bus waveguide, which further results in the stronger PIT effect. On the other hand, unlike other reported nanoribbon waveguides, our structures are formed by the local variation of chemical potential on the identical graphene monolayer, and this provides the easier integration with other functional components on the same material platform. Moreover, this plasmonic nanostructure can be used as refractive index sensor with high sensing sensibility. And the slow light effect with a large group delay is also realized in the PIT system. The proposed nanostructure paves a new way towards the realization of graphene-based on-chip integrated nanophotonic devices.
Coupled mode theory
Electromagnetically induced transparency
Finite element method
Refractive index unit
Surface plasmon polaritons
Wang T, Zhang Y, Hong Z, Han Z (2014) Analogue of electromagnetically induced transparency in integrated plasmonics with radiative and subradiant resonators. Opt Express 22:21529–21534
Raza S, Bozhevolnyi S (2015) Slow-light plasmonic metamaterial based on dressed-state analog of electromagnetically induced transparency. Opt Lett 40:4253–4256
Han X, Wang T, Li X, Liu B, He Y, Tang J (2015) Dynamically tunable slow light based on plasmon induced transparency in disk resonators coupled MDM waveguide system. J Phys D Appl Phys 48:235102
Liu SD, Yang Z, Liu RP, Li XY (2011) Plasmonic-induced optical transparency in the near-infrared and visible range with double split nanoring cavity. Opt Express 19:15363–15370
Longdell JJ, Fraval E, Sellars MJ, Manson NB (2005) Stopped light with storage times greater than one second using electromagnetically induced transparency in a solid. Phys Rev Lett 95:063601
Li BX, Li HJ, Zeng LL, Zhan SP, He ZH, Chen ZQ, Xu H (2015) High-sensitivity sensing based on plasmon-induced transparency. IEEE Photonics J 7:1–7
Yan X, Wang T, Han X et al (2016) High sensitivity nanoplasmonic sensor based on plasmon-induced transparency in a graphene nanoribbon waveguide coupled with detuned graphene square-nanoring resonators. Plasmonics 1–7. doi:10.1007/s11468-016-0405-0.
Barnes WL, Dereux A, Ebbesen TW (2003) Surface plasmon subwavelength optics. Nature 424:824–830
Ditlbacher H, Krenn JR, Schider G, Leitner A, Aussenegg FR (2002) Two-dimensional optics with surface plasmon polaritons. Appl Phys Lett 81:1762–1764
Han Z, Bozhevolnyi SI (2011) Plasmon-induced transparency with detuned ultracompact Fabry-Perot resonators in integrated plasmonic devices. Opt Express 19:3251–3257
Zhu Y, Hu X, Yang H, Gong Q (2014) On-chip plasmon-induced transparency based on plasmonic coupled nanocavities. Sci Rep 4:03752
Lai G, Liang R, Zhang Y, Bian Z, Yi L, Zhan G, Zhao R (2015) Double plasmonic nanodisks design for electromagnetically induced transparency and slow light. Opt Express 23:6554–6561
Lu H, Liu X, Mao D (2012) Plasmonic analog of electromagnetically induced transparency in multi-nanoresonator-coupled waveguide systems. Phys Rev A 85:053803
Chen Z, Dai L, Jiang C (2011) Polarization-independent plasmon-induced transparency for plasmonic sensing. J Phys D Appl Phys 44:325106
Yang X, Yu M, Kwong DL, Wong CW (2010) Coupled resonances in multiple silicon photonic crystal cavities in all-optical solid-state analogy to electromagnetically induced transparency. IEEE J Sel Top Quantum Electron 16:288–294
Yang X, Yang J, Hu X, Zhu Y, Yang H, Gong Q (2015) Multilayer-WS2: ferroelectric composite for ultrafast tunable metamaterial-induced transparency applications. Appl Phys Lett 107:081110
Zhang S, Genov DA, Wang Y, Liu M, Zhang X (2008) Plasmon-induced transparency in metamaterials. Phys Rev Lett 101:047401
Grigorenko AN, Marco P, Novoselov KS (2012) Graphene plasmonics. Nat Photonics 6:749–758
Koppens FH, Chang DE, Garcia de Abajo FJ (2011) Graphene plasmonics: a platform for strong light-matter interaction. Nano Lett 11:3370–3377
Xiao S, Wang T, Jiang X, Yan X et al (2017) Strong interaction between graphene layer and Fano resonance in terahertz metamaterials. J Phys D Appl Phys 50(19):195101
Xiao S, Wang T, Liu Y et al (2016) Tunable light trapping and absorption enhancement with graphene ring arrays. Phys Chem Chem Phys 18(38):26661–26669
Qiu W, Liu X, Zhao J, He S, Ma Y, Wang J, Pan J (2014) Nanofocusing of mid-infrared electromagnetic waves on graphene monolayer. Appl Phys Lett 104:41109
Avouris P (2010) Graphene: electronic and photonic properties and devices. Nano Lett 10:4285–4294
Fei Z, Rodin AS, Andreev GO, Bao W, McLeod AS, Wagner M, Zhang LM, Zhao Z, Thiemens M, Dominguez G, Fogler MM, Neto AHC, Lau CN, Keilmann F, Basov DN (2012) Gate-tuning of graphene plasmons revealed by infrared nano-imaging. Nature 487:82–85
Chen J, Badioli M, Alonso-González P, Thongrattanasiri S, Huth F, Osmond J, Spasenović M, Centeno A, Pesquera A, Godignon P, Zurutuza Elorza A, Camara N, de Abajo FJG, Hillenbrand R, Koppens FHL (2012) Optical nano-imaging of gate-tunable graphene plasmons. Nature 487:77–81
Wang X, Xia X, Wang J, Zhang F, Hu ZD, Liu C (2015) Tunable plasmonically induced transparency with unsymmetrical graphene-ring resonators. J Appl Phys 118:013101
Xia X, Wang J, Zhang F, Hu ZD, Liu C, Yan X, Yuan L (2015) Multi-mode plasmonically induced transparency in dual coupled graphene-integrated ring resonators. Plasmonics 10:1409–1415
Han X, Wang T, Li X, Xiao S, Zhu Y (2015) Dynamically tunable plasmon induced transparency in a graphene-based nanoribbon waveguide coupled with graphene rectangular resonators structure on sapphire substrate. Opt Express 23:31945–31955
Li HJ, Wang LL, Zhang BH, Zhai X (2015) Tunable edge-mode-based mid-infrared plasmonically induced transparency in the coupling system of coplanar graphene ribbons. Appl Phys Express 9:012001
Sun C, Si J, Dong Z, Deng X (2016) Tunable multispectral plasmon induced transparency based on graphene metamaterials. Opt Express 24:11466–11474
Cheng H, Chen S, Yu P, Duan X, Xie B, Tian J (2013) Dynamically tunable plasmonically induced transparency in periodically patterned graphene nanostrips. Appl Phys Lett 103:203112
Shang XJ, Zhai X, Li XF, Wang LL, Wang BX, Liu GD (2016) Realization of graphene-based tunable plasmon-induced transparency by the dipole-dipole coupling. Plasmonics 11:419–423
Qiu M (2002) Effective index method for heterostructure-slab-waveguide-based two-dimensional photonic crystals. Appl Phys Lett 7:1163–1165
Fujita M, Sakai A, Baba T (1999) Ultrasmall and ultralow threshold GaInAsP–InP microdisk injection lasers: design, fabrication, lasing characteristics, and spontaneous emission factor. IEEE J Sel Top Quantum Electron 3:673–681
Bozhevolnyi SI (2006) Effective-index modeling of channel plasmon polaritons. Opt Express 14:9467–9476
Zhao J, Qiu W, Huang Y, Wang J, Kan Q, Pan J (2014) Investigation of plasmonic whispering-gallery mode characteristics for graphene. Opt Lett 39:5527–5530
Zhao J, Liu X, Qiu W, Ma Y, Huang Y, Wang J, Qiang K, Pan J (2014) Surface-plasmon-polariton whispering-gallery mode analysis of the graphene monolayer coated InGaAs nanowire cavity. Opt Express 22:5754
Qiu W, Liu X, Zhao J, Huang Y, Chen H, Li B, Wang J, Kan Q, Pan J (2015) Ultrabroad band rainbow capture and releasing in graded chemical potential distributed graphene monolayer. Plasmonics 10:1023–1028
Qiu P, Qiu W, Lin Z, Chen H, Tang Y, Wang JX, Pan JQ (2016) Investigation of the band structure of graphene-based plasmonic photonic crystals. Nanomaterials 6:166
Mikhailov SA, Ziegler K (2007) New electromagnetic mode in graphene. Phys Rev Lett 99:016803
Bolotin KI, Sikes KJ, Jiang Z, Klima M, Fudenberg G, Hone J, Stormer HL (2008) Ultrahigh electron mobility in suspended graphene. Solid State Commun 146:351–355
Haus HA, Huang W (1991) Coupled-mode theory. Proc IEEE Inst Electr Electron Eng 79:1505–1518
Hu M, Wang F, Liang R, Zhou S, Xiao L (2015) Plasmonic-induced transparency based on plasmonic asymmetric dual side-coupled cavities. Phys Lett A 379:581–584
The authors are grateful to the support by the Natural Science Fund of China under Grant No. 61378058, the Science and Technology Fund of Quanzhou under Grant No. Z1424009, the Fujian Province Science Funds for Distinguished Young Scholar (No. 2015J06015), the Promotion Program for Young and Middle-Aged Teachers in Science and Technology Research of Huaqiao University (No. ZQN-YX203), and the Project for Cultivating Postgraduates’ Innovative Ability in Scientific Research of Huaqiao University (1511301022).
WQ provided the original idea; PQ and HC designed the models; PQ and JR performed the simulations; PQ, ZL, JXW, QK, and JQP analyzed the data; PQ and WQ wrote the paper. All authors read and approved the final manuscript.
The authors declare that they have no competing interests.
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