2004
DOI: 10.1103/physrevlett.92.166801
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Quantum Shuttle Phenomena in a Nanoelectromechanical Single-Electron Transistor

Abstract: An analytical analysis of quantum shuttle phenomena in a nanoelectromechanical single-electron transistor has been performed in the realistic case, when the electron tunneling length is much greater than the amplitude of the zero point oscillations of the central island. It is shown that when the dissipation is below a certain threshold value, the vibrational ground state of the central island is unstable. The steady state into which this instability develops is studied. It is found that if the electric field … Show more

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Cited by 85 publications
(109 citation statements)
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“…[3,4,5]. They have also been extensively investigated theoretically [6,7,8,9,10].Another rapidly developing branch of condensed matter physics is spintronics [11], which deals with devices whose functionality depends on the control and manipulation of the spin rather than the charge of electrons. A recent development of great interest in this context is the demonstration of a magnetic hybrid nanostructure consisting of a single C 60 -molecule placed between two ferromagnetic electrodes [12].…”
mentioning
confidence: 99%
“…[3,4,5]. They have also been extensively investigated theoretically [6,7,8,9,10].Another rapidly developing branch of condensed matter physics is spintronics [11], which deals with devices whose functionality depends on the control and manipulation of the spin rather than the charge of electrons. A recent development of great interest in this context is the demonstration of a magnetic hybrid nanostructure consisting of a single C 60 -molecule placed between two ferromagnetic electrodes [12].…”
mentioning
confidence: 99%
“…For this we consider the time evolution of the expectation value of the coordinate,x(t) = Tr{xρ + }, and the momentum operators,p(t) = Tr{pρ + }, of the island (here ρ + ≡ ρ 0 + ρ 1 ). To first order in λ −1 , for symmetric tunneling couplings Γ L (0) = Γ R (0) = Γ/2 and in the high bias voltage limit (µ L − µ R = eV → ∞) the equations of motion for the first vibrational moments become closed, so that [13]…”
Section: A Shuttle Instability In the Quantum Regime Of Coulomb Blocmentioning
confidence: 99%
“…If the dissipation rate γ is below the threshold value γ thr = Γd/[λ(Γ 2 ) + 1], then the expectation value of the dot coordinate grows exponentially in time and the vibrational ground state is unstable. It was shown [13] that this exponential increase of the displacement drives the system into the nonlinear regime of the vibration dynamics, where the system reaches a stable steady state of developed shuttle motion.…”
Section: A Shuttle Instability In the Quantum Regime Of Coulomb Blocmentioning
confidence: 99%
“…As a consequence, a dc current through the system, induced by the voltage drop between the electrodes, becomes proportional to the frequency of the mechanical oscillations 1 . The idea of shuttle phenomena was also extended to the quantum realm [8][9][10][11] . Nanoelectromechanical shuttle systems have been also studied in the regime of ac excitation and several interesting effects on the transport properties and the dynamics of the shuttle system have been found [12][13][14][15][16] .…”
mentioning
confidence: 99%
“…As a consequence, a dc current through the system, induced by the voltage drop between the electrodes, becomes proportional to the frequency of the mechanical oscillations 1 . The idea of shuttle phenomena was also extended to the quantum realm [8][9][10][11] .…”
mentioning
confidence: 99%