2011
DOI: 10.1088/1742-6596/302/1/012001
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A Carbon Nanotube-based NEMS Parametric Amplifier for Enhanced Radio Wave Detection and Electronic Signal Amplification

Abstract: We propose a scheme for a parametric amplifier based on a single suspended carbon nanotube field-emitter. This novel electromechanical nanotube device acts as a phase-sensitive, variable-gain, band-pass-filtering amplifier for electronic signal processing and, at the same time, can operate as a variable-sensitivity, tuneable detector and transducer of radio frequency electromagnetic waves. The amplifier can exhibit infinite gain at pumping voltages much less than 10 Volts. Additionally, the amplifier's low ove… Show more

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Cited by 9 publications
(9 citation statements)
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“…Inspired by the Lorentz model for a bound electron in an oscillating field and by the behavior of a parametric oscillator, , we search for a theoretical description of the observed features of the induced net rotation in the simulations by cobbling together a linear out-of-phase response function at the characteristic frequency and an in-phase response function at twice the characteristic frequency, J = J max { τ 1 false( ω ω 0 false) 1 + [ 2 τ 1 false( ω ω 0 false) ] 2 + 1 1 + [ 2 τ 1 false( ω 2 ω 0 false) ] 2 } Rather amazingly this theory describes the frequency dependence of the net rotation quite well, as shown in Figure C. The response at the characteristic frequency arises from a direct driving of the phase (the equilibrium position in a harmonic approximation, Figure B), while the response at twice the characteristic frequency arises from parametric modulation of the amplitude (the spring constant in a harmonic approximation, Figure B).…”
Section: Discussionmentioning
confidence: 99%
“…Inspired by the Lorentz model for a bound electron in an oscillating field and by the behavior of a parametric oscillator, , we search for a theoretical description of the observed features of the induced net rotation in the simulations by cobbling together a linear out-of-phase response function at the characteristic frequency and an in-phase response function at twice the characteristic frequency, J = J max { τ 1 false( ω ω 0 false) 1 + [ 2 τ 1 false( ω ω 0 false) ] 2 + 1 1 + [ 2 τ 1 false( ω 2 ω 0 false) ] 2 } Rather amazingly this theory describes the frequency dependence of the net rotation quite well, as shown in Figure C. The response at the characteristic frequency arises from a direct driving of the phase (the equilibrium position in a harmonic approximation, Figure B), while the response at twice the characteristic frequency arises from parametric modulation of the amplitude (the spring constant in a harmonic approximation, Figure B).…”
Section: Discussionmentioning
confidence: 99%
“…Our first example deals with a carbon nanotube that is excited by an external electrical field. As discussed in , carbon nanotubes possess very unique and promising characteristics for use as NEMS resonators . In this study, we suppose that the carbon nanotube is a conductor.…”
Section: Numerical Examplesmentioning
confidence: 95%
“…As discussed in [31], carbon nanotubes possess very unique and promising characteristics for use as NEMS resonators [2,[52][53][54][55]. In this study, we suppose that the carbon nanotube is a conductor.…”
Section: Nanotube Vibrationmentioning
confidence: 97%
“…CNTs are the smallest scale nanomaterials that can be observed only by a transmission electron microscope (TEM). The excellent structural characteristics and the mechanical and physical properties make CNTs potential candidates for the next generation of nanoelectromechanical systems (NEMS) [11][12][13][14][15].…”
Section: Introductionmentioning
confidence: 99%