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1

Lee, Haw-Long, Yu-Ching Yang, and Win-Jin Chang. "Atomic-Scale Finite Element Method for Analyzing the Sensitivity of Graphyne-Based Resonators." Journal of Nanomaterials 2018 (August 5, 2018): 1–6. http://dx.doi.org/10.1155/2018/2580171.

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An atomic-scale finite element method was applied to analyze the sensitivities of α-, β-, γ-, and 6,6,12-graphyne-based resonators in mass detection under different boundary conditions. These sensitivities are then compared with that of a graphene-based resonator obtained in a previous study. According to the analysis results, among the graphyne-based resonators, the α type shows the highest sensitivity, while the γ type shows the lowest. In addition, the sensitivity decreases as the resonator size increases. We also find that the location of the attached mass has a significant effect on the s
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2

Liu, Ying, Jia Peng Zhen, Wen Xiang Yang, et al. "Research on Dissipation Dilution Mechanism and Boundary Dissipation Suppression Technique for High-Stress Graphene Nanoelectromechanical Resonator." Journal of Physics: Conference Series 2557, no. 1 (2023): 012064. http://dx.doi.org/10.1088/1742-6596/2557/1/012064.

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Abstract The low-quality factor is a key bottleneck for the engineering and commercial application of graphene nanoelectromechanical resonators at room temperature. The hypothesis in dissipation dominated by the ohmic loss is difficult to cover this phenomenon. Mechanical loss may still be on the list of the main causes for the quality factor stress-modulation characteristics of graphene resonators. The dissipation dilution theory reveals the intrinsic energy and dissipation mechanism of the traditional high-stress silicon-based resonator, which may also be applied to two-dimensional (2D) mate
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3

Kim, Chang-Wan, Mai Duc Dai, and Kilho Eom. "Finite-size effect on the dynamic and sensing performances of graphene resonators: the role of edge stress." Beilstein Journal of Nanotechnology 7 (May 9, 2016): 685–96. http://dx.doi.org/10.3762/bjnano.7.61.

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We have studied the finite-size effect on the dynamic behavior of graphene resonators and their applications in atomic mass detection using a continuum elastic model such as modified plate theory. In particular, we developed a model based on von Karman plate theory with including the edge stress, which arises from the imbalance between the coordination numbers of bulk atoms and edge atoms of graphene. It is shown that as the size of a graphene resonator decreases, the edge stress depending on the edge structure of a graphene resonator plays a critical role on both its dynamic and sensing perfo
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4

Nam, Man Hoai, Bui Son Tung, Bui Xuan Khuyen, et al. "Graphene-Integrated Plasmonic Metamaterial for Manipulation of Multi-Band Absorption, Based on Near-Field Coupled Resonators." Crystals 12, no. 4 (2022): 525. http://dx.doi.org/10.3390/cryst12040525.

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We demonstrated a multi-band plasmonic metamaterial absorber (MA), based on the near-field coupled resonators. In addition to the individual resonances of resonators in the proposed structure, which were split-ring resonator (SRR) and cross-shape structures, another resonance was also excited owing to the coupling of resonators, revealing a triple-band absorption. Furthermore, to control the absorption behavior, on the top of the SRRs, the identical SRRs made of graphene ink were pasted. By increasing the resistance of graphene ink, the coupling strength was weakened, changing the triple-band
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5

Zhang, Zhuo-Zhi, Xiang-Xiang Song, Gang Luo, et al. "Coherent phonon dynamics in spatially separated graphene mechanical resonators." Proceedings of the National Academy of Sciences 117, no. 11 (2020): 5582–87. http://dx.doi.org/10.1073/pnas.1916978117.

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Vibrational modes in mechanical resonators provide a promising candidate to interface and manipulate classical and quantum information. The observation of coherent dynamics between distant mechanical resonators can be a key step toward scalable phonon-based applications. Here we report tunable coherent phonon dynamics with an architecture comprising three graphene mechanical resonators coupled in series, where all resonators can be manipulated by electrical signals on control gates. We demonstrate coherent Rabi oscillations between spatially separated resonators indirectly coupled via an inter
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6

Liu, Shen, Hang Xiao, Yanping Chen, et al. "Nano-Optomechanical Resonators Based on Suspended Graphene for Thermal Stress Sensing." Sensors 22, no. 23 (2022): 9068. http://dx.doi.org/10.3390/s22239068.

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Nanomechanical resonators made from suspended graphene combine the properties of ultracompactness and ultrahigh detection sensitivity, making them interesting devices for sensing applications. However, nanomechanical systems can be affected by membrane stress. The present work developed an optomechanical resonator for thermal stress sensing. The proposed resonator consists of a section of hollow core fiber (HCF) and a trampoline graphene–Au membrane. An all-optical system that integrated optical excitation and optical detection was applied. Then, the resonance frequency of the resonator was ob
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7

Liu, Yujian, Cheng Li, Shangchun Fan, Xuefeng Song, and Zhen Wan. "The Effect of Annealing and Optical Radiation Treatment on Graphene Resonators." Nanomaterials 12, no. 15 (2022): 2725. http://dx.doi.org/10.3390/nano12152725.

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Graphene resonant sensors have shown strong competitiveness with respect to sensitivity and size. To advance the applications of graphene resonant sensors, the damage behaviors of graphene harmonic oscillators after thermal annealing and laser irradiation were investigated by morphology analysis and frequency domain vibration characteristics. The interface stress was proven to be the key factor that directly affected the yield of resonators. The resulting phenomenon could be improved by appropriately controlling the annealing temperature and size of resonators, thereby achieving membrane intac
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8

Wang, Zhenqiang, Mingqing Yang, and Junhui He. "Sensing Properties of GO and Amine-Silica Nanoparticles Functionalized QCM Sensors for Detection of Formaldehyde." International Journal of Nanoscience 13, no. 05n06 (2014): 1460011. http://dx.doi.org/10.1142/s0219581x14600114.

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In the current work, graphene oxides (GO) and Amine-Functionalized Silica Nanoparticles ( NH 2-SNs) were used as sensing layer on quart crystal microbalance (QCM) for detection of HCHO gas. The GO and NH 2-SNs functionalized QCM resonators all had a significant response to HCHO gas. The sensitivity of GO functionalized QCM resonator is 0.04 Hz/(μg⋅ppm), which is four times as high as that of NH 2-SNs functionalized QCM resonator (0.01 Hz/(μg⋅ppm)). The GO functionalized QCM resonators would be of benefit in area of environmental applications.
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9

Xiao, Yang, Fang Luo, Yuchen Zhang, Feng Hu, Mengjian Zhu, and Shiqiao Qin. "A Review on Graphene-Based Nano-Electromechanical Resonators: Fabrication, Performance, and Applications." Micromachines 13, no. 2 (2022): 215. http://dx.doi.org/10.3390/mi13020215.

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The emergence of graphene and other two-dimensional materials overcomes the limitation in the characteristic size of silicon-based micro-resonators and paved the way in the realization of nano-mechanical resonators. In this paper, we review the progress to date of the research on the fabrication methods, resonant performance, and device applications of graphene-based nano-mechanical resonators, from theoretical simulation to experimental results, and summarize both the excitation and detection schemes of graphene resonators. In recent years, the applications of graphene resonators such as mass
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10

Chen, Ting, Tianyu Xiang, Jianwei Wang, Mingxing Xu, and Tao Lei. "Tunable toroidal resonance based on hybrid graphene-metal metasurfaces." Journal of Applied Physics 132, no. 16 (2022): 165103. http://dx.doi.org/10.1063/5.0104043.

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With the rise of artificial magnetism and metamaterials, toroidal resonance has gained much attention for its special properties. In this paper, we propose a novel hybrid graphene-metal metamolecule consisting of a square bracket-like resonator and two asymmetric U-shaped resonators. By applying various Fermi energies to graphene, the amplitude of electromagnetically induced transparency (EIT) can be efficiently manipulated, and the maximum amplitude modulation depth can attain 81% in the microwave region. Numerical simulations and theoretical analysis demonstrate that the dynamic manipulation
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11

Ma, Qichang, Jianan Dai, Aiping Luo, and Weiyi Hong. "Numerical and Theoretical Study of Tunable Plasmonically Induced Transparency Effect Based on Bright–Dark Mode Coupling in Graphene Metasurface." Nanomaterials 10, no. 2 (2020): 232. http://dx.doi.org/10.3390/nano10020232.

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In this paper, we numerically and theoretically study the tunable plasmonically induced transparency (PIT) effect based on the graphene metasurface structure consisting of a graphene cut wire (CW) resonator and double split-ring resonators (SRRs) in the middle infrared region (MIR). Both the theoretical calculations according to the coupled harmonic oscillator model and simulation results indicate that the realization of the PIT effect significantly depends on the coupling distance and the coupling strength between the CW resonator and SRRs. In addition, the geometrical parameters of the CW re
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12

Xiao, Xing, Shang-Chun Fan, and Cheng Li. "The Effect of Edge Mode on Mass Sensing for Strained Graphene Resonators." Micromachines 12, no. 2 (2021): 189. http://dx.doi.org/10.3390/mi12020189.

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Edge mode could disturb the ultra-subtle mass detection for graphene resonators. Herein, classical molecular dynamics simulations are performed to investigate the effect of edge mode on mass sensing for a doubly clamped strained graphene resonator. Compared with the fundamental mode, the localized vibration of edge mode shows a lower frequency with a constant frequency gap of 32.6 GHz, despite the mutable inner stress ranging from 10 to 50 GPa. Furthermore, the resonant frequency of edge mode is found to be insensitive to centrally located adsorbed mass, while the frequency of the fundamental
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13

Wang, Jicheng, Baojie Tang, Xiushan Xia, and Shutian Liu. "Active Multiple Plasmon-Induced Transparency with Graphene Sheets Resonators in Mid-Infrared Frequencies." Journal of Nanomaterials 2016 (2016): 1–8. http://dx.doi.org/10.1155/2016/3678578.

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A multiple plasmon-induced transparency (PIT) device operated in the mid-infrared region has been proposed. The designed model is comprised of one graphene ribbon as main waveguide and two narrow graphene sheets resonators. The phase coupling between two graphene resonators has been investigated. The multimode PIT resonances have been found in both cases and can be dynamically tuned via varying the chemical potential of graphene resonators without optimizing its geometric parameters. In addition, this structure can get multiple PIT effect by equipping extra two sheets on the symmetric position
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14

Wen, Chunchao, Jie Luo, Wei Xu, Zhihong Zhu, Shiqiao Qin, and Jianfa Zhang. "Enhanced Molecular Infrared Spectroscopy Employing Bilayer Graphene Acoustic Plasmon Resonator." Biosensors 11, no. 11 (2021): 431. http://dx.doi.org/10.3390/bios11110431.

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Graphene plasmon resonators with the ability to support plasmonic resonances in the infrared region make them a promising platform for plasmon-enhanced spectroscopy techniques. Here we propose a resonant graphene plasmonic system for infrared spectroscopy sensing that consists of continuous graphene and graphene ribbons separated by a nanometric gap. Such a bilayer graphene resonator can support acoustic graphene plasmons (AGPs) that provide ultraconfined electromagnetic fields and strong field enhancement inside the nano-gap. This allows us to selectively enhance the infrared absorption of pr
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15

Fan, Shang-Chun, Yang Lu, Peng-Cheng Zhao, Fu-Tao Shi, Zhan-She Guo, and Wei-Wei Xing. "Research Progress of Graphene Nano-Electromechanical Resonant Sensors—A Review." Micromachines 13, no. 2 (2022): 241. http://dx.doi.org/10.3390/mi13020241.

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Graphene nano-electromechanical resonant sensors have wide application in areas such as seawater desalination, new energy, biotechnology, and aerospace due to their small size, light weight, and high sensitivity and resolution. This review first introduces the physical and chemical properties of graphene and the research progress of four preparation processes of graphene. Next, the principle prototype of graphene resonators is analyzed, and three main methods for analyzing the vibration characteristics of a graphene resonant sheet are described: molecular structural mechanics, non-local elasti
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16

Xiao, Yang, Feng Hu, Mengjian Zhu, et al. "Effect of induced current loss on quality factor of graphene resonators." AIP Advances 12, no. 3 (2022): 035041. http://dx.doi.org/10.1063/5.0082259.

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As the important electric loss of a graphene resonator, intrinsic current loss has received increasing attention, but the existing research is limited to qualitative analysis and approximate calculation. Based on the microscopic behavior of carriers, we have accurately established the calculation model of induced current loss, which is in good agreement with the existing experimental results. Compared with the previous models, the model in this work can not only fit the inverse V-shaped Q − V dc curve well but also be compatible with the V-shaped Q − V dc curve, which is beyond the reach of th
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17

Jokic, Ivana, Milos Frantlovic, Zoran Djuric, and Miroslav Dukic. "RF MEMS/NEMS resonators for wireless communication systems and adsorption-desorption phase noise." Facta universitatis - series: Electronics and Energetics 28, no. 3 (2015): 345–81. http://dx.doi.org/10.2298/fuee1503345j.

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During the past two decades a considerable effort has been made to develop radio-frequency (RF) resonators which are fabricated using the micro/nanoelectro-mechanical systems (MEMS/NEMS) technologies, in order to replace conventional large off-chip components in wireless transceivers and other high-speed electronic systems. The first part of the paper presents an overview of RF MEMS and NEMS resonators, including those based on two-dimensional crystals (e.g. graphene). The frequency tuning in MEMS/NEMS resonators is then analyzed. Improvements that would be necessary in order for MEMS/NEMS res
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18

Szuromi, P. "MATERIALS SCIENCE: Graphene Oxide Resonators." Science 322, no. 5904 (2008): 1026b. http://dx.doi.org/10.1126/science.322.5904.1026b.

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19

Bunch, J. S., A. M. van der Zande, S. S. Verbridge, et al. "Electromechanical Resonators from Graphene Sheets." Science 315, no. 5811 (2007): 490–93. http://dx.doi.org/10.1126/science.1136836.

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20

Majumdar, A., Jonghwan Kim, J. Vuckovic, and Feng Wang. "Graphene for Tunable Nanophotonic Resonators." IEEE Journal of Selected Topics in Quantum Electronics 20, no. 1 (2014): 68–71. http://dx.doi.org/10.1109/jstqe.2013.2273413.

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21

Ye, Fan, Jaesung Lee, and Philip X. L. Feng. "Atomic layer MoS2-graphene van der Waals heterostructure nanomechanical resonators." Nanoscale 9, no. 46 (2017): 18208–15. http://dx.doi.org/10.1039/c7nr04940d.

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We have realized the first MoS<sub>2</sub>-graphene heterostructure nanomechanical resonators with varying thickness and size. Comparing experimental results and theoretical calculations, we have quantified the tension levels in these heterostructure 2D resonators.
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22

Wang, Yueke, Xinru Shen, and Quansheng Chen. "Tunable plasmon-induced transparency with graphene-sheet structure." Modern Physics Letters B 30, no. 19 (2016): 1650232. http://dx.doi.org/10.1142/s0217984916502328.

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We investigate theoretically and numerically the tunable plasmon-induced transparency (PIT) phenomenon in graphene-sheet system in infrared range. We show that when surface plasmon polaritons (SPPs) propagate along a monolayer graphene sheet with two detuned side-coupled resonators, the PIT-like transmission spectra of SPPs appear. Thanks to the tunable permittivity of graphene by bias voltages, the resonant wavelength of side-coupled resonators can be changed. So the transmission spectra can be tuned dynamically and the tunable PIT phenomenon is achieved. Numerical simulation by finite elemen
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23

Han, Chen, Renbin Zhong, Zekun Liang, et al. "Independently Tunable Multipurpose Absorber with Single Layer of Metal-Graphene Metamaterials." Materials 14, no. 2 (2021): 284. http://dx.doi.org/10.3390/ma14020284.

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This paper reports an independently tunable graphene-based metamaterial absorber (GMA) designed by etching two cascaded resonators with dissimilar sizes in the unit cell. Two perfect absorption peaks were obtained at 6.94 and 10.68 μm with simple single-layer metal-graphene metamaterials; the peaks show absorption values higher than 99%. The mechanism of absorption was analyzed theoretically. The independent tunability of the metamaterial absorber (MA) was realized by varying the Fermi level of graphene under a set of resonators. Furthermore, multi-band and wide-band absorption were observed b
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24

Han, Chen, Renbin Zhong, Zekun Liang, et al. "Independently Tunable Multipurpose Absorber with Single Layer of Metal-Graphene Metamaterials." Materials 14, no. 2 (2021): 284. http://dx.doi.org/10.3390/ma14020284.

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This paper reports an independently tunable graphene-based metamaterial absorber (GMA) designed by etching two cascaded resonators with dissimilar sizes in the unit cell. Two perfect absorption peaks were obtained at 6.94 and 10.68 μm with simple single-layer metal-graphene metamaterials; the peaks show absorption values higher than 99%. The mechanism of absorption was analyzed theoretically. The independent tunability of the metamaterial absorber (MA) was realized by varying the Fermi level of graphene under a set of resonators. Furthermore, multi-band and wide-band absorption were observed b
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25

Sun, Haoying, Lin Zhao, Jinsong Dai, et al. "Broadband Filter and Adjustable Extinction Ratio Modulator Based on Metal-Graphene Hybrid Metamaterials." Nanomaterials 10, no. 7 (2020): 1359. http://dx.doi.org/10.3390/nano10071359.

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A novel multifunctional device based on a hybrid metal–graphene Electromagnetically induced transparency (EIT) metamaterial at the terahertz band is proposed. It is composed of a parallel cut wire pair (PCWP) that serves as a dark mode resonator, a vertical cut wire pair (VCWP) that serves as a bright mode resonator and a graphene ribbon that serves as a modulator. An ultra-broadband transmission window with 1.23 THz bandwidth can be obtained. The spectral extinction ratio can be tuned from 26% to 98% by changing the Fermi level of the graphene. Compared with previous work, our work has superi
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26

He, Xunjun, Yiming Huang, Xingyu Yang, Lei Zhu, Fengmin Wu, and Jiuxing Jiang. "Tunable electromagnetically induced transparency based on terahertz graphene metamaterial." RSC Advances 7, no. 64 (2017): 40321–26. http://dx.doi.org/10.1039/c7ra06770d.

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The terahertz EIT graphene metamaterial, consisting of two coupled split ring resonators placed in orthogonally twisted fashion, was proposed by patterning graphene. An actively controlled EIT peak can be obtained by changing relaxation time or Fermi energy of graphene.
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27

Chen, Jianzhong, Jiali Zhang, Yutong Zhao, et al. "High-Selectivity Bandpass Filter with Controllable Attenuation Based on Graphene Nanoplates." Materials 15, no. 5 (2022): 1694. http://dx.doi.org/10.3390/ma15051694.

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A high-selectivity band pass filter with controllable attenuation based on graphene nanoplates is proposed in this paper. Graphene with controllable resistance has a good uniform attenuation effect to electric field intensity. The filter utilizes quarter wavelength stepped impedance resonators and mixed electromagnetic coupling to have compact circuits and high performance. The graphene nanoplates are loaded on the microstrip resonator to reduce the electric field intensity, which results in a flat attenuation in the passband. In addition, the filter has two transmission zeros, which lead to a
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28

Ye, Yichen, Tingting Song, Yiyuan Xie, and Chuandong Li. "Design of All-Optical Subtractors Utilized with Plasmonic Ring Resonators for Optical Computing." Photonics 10, no. 7 (2023): 724. http://dx.doi.org/10.3390/photonics10070724.

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In this paper, a novel plasmonic all-optical half-subtractor and full-subtractor are designed for optical computing. The structure of plasmonic subtractors consists of a metal–insulator–metal (MIM) waveguide and rectangular ring resonators covered by a graphene layer. Due to the nonlinear optical properties of graphene, the states of the plasmonic resonators can be controlled by the pump intensity of a pump beam focused on the graphene layer. The resonators can work as all-optical switches with an ultra-fast response time to constitute optical logic devices according to the directed logic mech
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29

Atalaya, Juan, Andreas Isacsson, and Jari M. Kinaret. "Continuum Elastic Modeling of Graphene Resonators." Nano Letters 8, no. 12 (2008): 4196–200. http://dx.doi.org/10.1021/nl801733d.

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Sharma, Ankur, Utkarshaa Varshney, and Yuerui Lu. "Electronic applications of graphene mechanical resonators." IET Circuits, Devices & Systems 9, no. 6 (2015): 413–19. http://dx.doi.org/10.1049/iet-cds.2015.0134.

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Low, Tony, Yongjin Jiang, Mikhail Katsnelson, and Francisco Guinea. "Electron Pumping in Graphene Mechanical Resonators." Nano Letters 12, no. 2 (2012): 850–54. http://dx.doi.org/10.1021/nl2038985.

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32

Verbiest, Gerard J., Jan N. Kirchhof, Jens Sonntag, Matthias Goldsche, Tymofiy Khodkov, and Christoph Stampfer. "Detecting Ultrasound Vibrations with Graphene Resonators." Nano Letters 18, no. 8 (2018): 5132–37. http://dx.doi.org/10.1021/acs.nanolett.8b02036.

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Wang, Xianjun, Hongyun Meng, Shuying Deng, et al. "Hybrid Metal Graphene-Based Tunable Plasmon-Induced Transparency in Terahertz Metasurface." Nanomaterials 9, no. 3 (2019): 385. http://dx.doi.org/10.3390/nano9030385.

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In this paper, we look at the work of a classical plasmon-induced transparency (PIT) based on metasurface, including a periodic lattice with a cut wire (CW) and a pair of symmetry split ring resonators (SSR). Destructive interference of the ‘bright-dark’ mode originated from the CW and a pair of SSRs and resulted in a pronounced transparency peak at 1.148 THz, with 85% spectral contrast ratio. In the simulation, the effects of the relative distance between the CW and the SSR pair resonator, as well as the vertical distance of the split gap, on the coupling strength of the PIT effect, have been
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Li, Wenhua, and Wenchao Tian. "Molecular Dynamics Analysis of Graphene Nanoelectromechanical Resonators Based on Vacancy Defects." Nanomaterials 12, no. 10 (2022): 1722. http://dx.doi.org/10.3390/nano12101722.

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Due to the limitation of graphene processing technology, the prepared graphene inevitably contains various defects. The defects will have a particular influence on the macroscopic characteristics of the graphene. In this paper, the defect-based graphene nanoresonators are studied. In this study, the resonant properties of graphene were investigated via molecular dynamic simulations. The effect of vacancy defects and hole defects at different positions, numbers, and concentrations on the resonance frequency of graphene nanoribbons was studied. The results indicated that single monatomic vacancy
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Jung, Minkyung, Peter Rickhaus, Simon Zihlmann, Alexander Eichler, Peter Makk, and Christian Schönenberger. "GHz nanomechanical resonator in an ultraclean suspended graphene p–n junction." Nanoscale 11, no. 10 (2019): 4355–61. http://dx.doi.org/10.1039/c8nr09963d.

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Yuan, Chenzhi, Wei Zhang, and Yidong Huang. "Photothermal effect in graphene-coated microsphere resonators." Applied Physics Express 11, no. 7 (2018): 072503. http://dx.doi.org/10.7567/apex.11.072503.

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Jung, Suyong. "Whispering-gallery mode quantum resonators in graphene." NPG Asia Materials 7, no. 10 (2015): e218-e218. http://dx.doi.org/10.1038/am.2015.106.

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Guan, Fen, Piranavan Kumaravadivel, Dmitri V. Averin, and Xu Du. "Tuning strain in flexible graphene nanoelectromechanical resonators." Applied Physics Letters 107, no. 19 (2015): 193102. http://dx.doi.org/10.1063/1.4935239.

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Kang, Jeong Won, Jun Ha Lee, Ho Jung Hwang, and Ki-Sub Kim. "Developing accelerometer based on graphene nanoribbon resonators." Physics Letters A 376, no. 45 (2012): 3248–55. http://dx.doi.org/10.1016/j.physleta.2012.08.040.

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40

Grady, Eldad, Enrico Mastropaolo, Tao Chen, Andrew Bunting, and Rebecca Cheung. "Low frequency graphene resonators for acoustic sensing." Microelectronic Engineering 119 (May 2014): 105–8. http://dx.doi.org/10.1016/j.mee.2014.02.036.

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41

Alemán, Benjamín, Michael Rousseas, Yisheng Yang, et al. "Polymer-free, low tension graphene mechanical resonators." physica status solidi (RRL) - Rapid Research Letters 7, no. 12 (2013): 1064–66. http://dx.doi.org/10.1002/pssr.201300087.

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42

Lao, Chaode, Yaoyao Liang, Xianjun Wang, et al. "Dynamically Tunable Resonant Strength in Electromagnetically Induced Transparency (EIT) Analogue by Hybrid Metal-Graphene Metamaterials." Nanomaterials 9, no. 2 (2019): 171. http://dx.doi.org/10.3390/nano9020171.

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In this paper, a novel method to realize a dynamically tunable analogue of EIT for the resonance strength rather than the resonance frequency is proposed in the terahertz spectrum. The introduced method is composed of a metal EIT-like structure, in which a distinct EIT phenomenon resulting from the near field coupling between bright and dark mode resonators can be obtained, as well as an integrated monolayer graphene ribbon under the dark mode resonator that can continuously adjust the resonance strength of transparency peak by changing the Fermi level of the graphene. Comparing structures tha
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43

Huang, Yu, and Li Hua Wu. "Nonlinear TE-Polarized Surface Plasmons at the Interface between Graphene and Metamaterials." Advanced Materials Research 933 (May 2014): 47–51. http://dx.doi.org/10.4028/www.scientific.net/amr.933.47.

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Nonlinear TE-polarized surface plasmons localized at the interface between graphene and metamaterials are investigated analytically. The normalized momentum of graphene surface plasmons at the interface between graphene and metamaterials composed of arrays of wires and split-ring resonators (SRR) embedded into a nonlinear dielectric exhibits bistable behavior with the magnetic field intensity. The effect is explained by the hysteresis-type dependence of the nonlinear permeability of metamaterials on the field intensity.
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44

Zaitsev, Anton, Alexander Grebenchukov, and Mikhail Khodzitsky. "Tunable THz Graphene Filter Based on Cross-In-Square-Shaped Resonators Metasurface." Photonics 6, no. 4 (2019): 119. http://dx.doi.org/10.3390/photonics6040119.

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The tunable terahertz (THz) Fano-resonant filter based on hybrid metal-graphene metamaterial was proposed. The optical parameters of metasurface with unit cell in the form of a cross-shaped graphene sheet in the center of a square gold ring were simulated by the finite element method using a surface conductivity model of a graphene monolayer. The narrowband modulation of the transmission by varying the Fermi level of the graphene and the position of graphene cross inside the metal ring was demonstrated. Simulation results were well explained theoretically using a three-coupled oscillator model
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45

Ikeda, Taro, Etsumi Kojima, Shinya Sugiura, and Hideo Iizuka. "Reflective graphene metasurface without a metallic plate." Journal of Applied Physics 133, no. 7 (2023): 073102. http://dx.doi.org/10.1063/5.0134500.

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Reflective metasurfaces for arbitrary wave-front control require unit cells to achieve both [Formula: see text] phase rotation and unity amplitude in reflection waves, and such requirements are a fundamental challenge for ultra-thin metasurfaces without the use of a metallic plate. We analytically show that in two coupled resonators, tuning the resonance frequency with the external decay rate for one of the resonators enables near [Formula: see text] phase rotation and unity amplitude in the reflection wave, where no reflector is required. We implement the mechanism on a reflective graphene me
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46

Sun, Jian-Zhong, Le Zhang, and Fei Gao. "Ultra-compact terahertz switch with graphene ring resonators." Chinese Physics B 25, no. 10 (2016): 108701. http://dx.doi.org/10.1088/1674-1056/25/10/108701.

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47

Weber, P., J. Güttinger, I. Tsioutsios, D. E. Chang, and A. Bachtold. "Coupling Graphene Mechanical Resonators to Superconducting Microwave Cavities." Nano Letters 14, no. 5 (2014): 2854–60. http://dx.doi.org/10.1021/nl500879k.

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48

Schmid, Silvan, Tolga Bagci, Emil Zeuthen, et al. "Single-layer graphene on silicon nitride micromembrane resonators." Journal of Applied Physics 115, no. 5 (2014): 054513. http://dx.doi.org/10.1063/1.4862296.

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49

Xu, Yuehang, Changyao Chen, Vikram V. Deshpande, et al. "Radio frequency electrical transduction of graphene mechanical resonators." Applied Physics Letters 97, no. 24 (2010): 243111. http://dx.doi.org/10.1063/1.3528341.

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50

Thomas, S., M. Cole, A. De Luca, et al. "Graphene-coated Rayleigh SAW Resonators for NO2 Detection." Procedia Engineering 87 (2014): 999–1002. http://dx.doi.org/10.1016/j.proeng.2014.11.328.

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