2007
DOI: 10.1134/s1063783407100332
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Control of the motion of nanoelectromechanical systems based on carbon nanotubes

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Cited by 8 publications
(11 citation statements)
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“…We further demonstrate that the bridged-CNS-based nano-oscillators can be excited and driven by an external electric field, a crucial feature to enable their potential application in ultrafast NEMS devices. For the MWCNT-based nano-oscillators, it has been proposed that by inducing net charge [ 20 ] or electric dipole [ 18 ] into the inner tube, the carbon atoms in the charged/polarized inner tube are subjected to electrostatic capacitive force in an external electric field, which could be potentially used to initialize the oscillation. Controlled charging/polarization of the inner tube of an MWCNT requires manipulation with sub-nanometer precision, thus remains rather challenging to achieve experimentally.…”
Section: Resultsmentioning
confidence: 99%
“…We further demonstrate that the bridged-CNS-based nano-oscillators can be excited and driven by an external electric field, a crucial feature to enable their potential application in ultrafast NEMS devices. For the MWCNT-based nano-oscillators, it has been proposed that by inducing net charge [ 20 ] or electric dipole [ 18 ] into the inner tube, the carbon atoms in the charged/polarized inner tube are subjected to electrostatic capacitive force in an external electric field, which could be potentially used to initialize the oscillation. Controlled charging/polarization of the inner tube of an MWCNT requires manipulation with sub-nanometer precision, thus remains rather challenging to achieve experimentally.…”
Section: Resultsmentioning
confidence: 99%
“…We considered several DWNT oscillators of the length from 2.4 to 6.3 nm. The nanotube walls were equal in length [15]. Both ends of the outer wall were open and not functionalized, so that the telescopic extension of the inner wall was possible at both ends.…”
Section: Methodsmentioning
confidence: 99%
“…The relative dispersion of the energy loss E Δ over a half-period for the defect-free 3.1 nm (5,5)@(10,10) nanotube-based oscillator is about 1.5 at a temperature of 300 K. With the same initial telescopic extension of the inner wall of 30% of the nanotube length, the relative dispersion of the energy loss E Δ over a half-period is below 0.5 for the oscillator that is longer than 30 nm. We suppose that the fluctuations can influence the possibility of the controllable operation mode of the gigahertz oscillator (this operation mode is considered in [15]). Thus, the fluctuations impose restrictions on the minimum size of the nanotube-based NEMS that may be used in applications.…”
Section: Fluctuations In Nemsmentioning
confidence: 99%
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“…The detailed analysis shows that the critical amplitude F 0 min of the external control force is minimal in the case where lengths of inner and outer walls are equal. In this case the relationship for the gigahertz oscillator frequency (3) takes the form v5(p/2)(F W /2ms) 1/2 , t in 50 and equation (1) takes the form F 0 min 5 p 2 F W /32Q (9), where F W is the van der Waals force.…”
mentioning
confidence: 99%