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Parametric Instability of Mobile Elastic Gate in Tera- and Nano- High Electron Mobility Transistor V.L. Semenenko, V.G. Leiman, A.V. Arsenin, A.D. Gladun and V.I Ryzhii
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Outline Introduction Modulated THz radiation detector Reduction the model to the capacitance transducer equations Calculation for the threshold signal amplitude and power
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Motivation Expected roadmap for some THz applications, 2007*) * Masayoshi Tonouchi, “Cutting-edge terahertz technology”, Nature Photonics 1, 97 - 105 (2007) Modulated THz radiation detectors are required
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The first resonant gate transistor H. C. Nathanson, W. E. Newell, R. A. Wickstorm, and J. R. Davis, IEEE Trans. Electron Devices 14, 117, 1967.
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Recent modulated THz detectors V. Ryzhii, M. Ryzhii, Y. Hu, et al., Appl. Phys. Lett. 90, 203503 (2007). V. G. Leiman, et al., J. Appl. Phys. 104, 024514 (2008).
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Parametric instability in capacitance transducer Dimensionless equations
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Calculations for threshold Λ
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Device scheme & model Front viewTop view Gate charge field component Hydrodynamic model of electron transport in 2DEG
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Solution of the linearized equations Because of the linear equations Characteristic frequency & quality factor of the 2DEG oscillations
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Power consumption & linear force acting on the gate
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Equivalent system of ODEs … As it would be if the device was the following:
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Fitting the parameters C & D
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Dimensionless equations system
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Results & conclusion * Huttel A.K. et al // Nano Lett., Vol. 9, No. 7, P. 2547, 2009. ** Arsenin A.V. et al // J. of Comm. Tech. and Electronics,Vol. 54, No. 11, P. 1319, 2009. According to our previous work**), in the case of plain metallic cantilever gate: can be 2-3 orders lower in the case of SWCNT gate
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Thank you very much for your attention!
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Calculation for the values Θ res & Ψ res
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