273 research outputs found

    Laser-like Instabilities in Quantum Nano-electromechanical Systems

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    We discuss negative damping regimes in quantum nano-electromechanical systems formed by coupling a mechanical oscillator to a single-electron transistor (normal or superconducting). Using an analogy to a laser with a tunable atom-field coupling, we demonstrate how these effects scale with system parameters. We also discuss the fluctuation physics of both the oscillator and the single-electron transistor in this regime, and the degree to which the oscillator motion is coherent.Comment: 4+ pages, 1 figure; reference to the work of Dykman and Krivoglaz adde

    Using a qubit to measure photon number statistics of a driven, thermal oscillator

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    We demonstrate theoretically how photon number statistics of a driven, damped oscillator at finite temperature can be extracted by measuring the dephasing spectrum of a two-level system dispersively coupled to the oscillator; we thus extend the work of Dykman (1987) and Gambetta et al. (2006). We carefully consider the fidelity of this scheme-- to what extent does the measurement reflect the initial number statistics of the mode? We also derive analytic results for the dephasing of a qubit by a driven, thermal mode, and compare results obtained at different levels of approximation. Our results have relevance both to experiments in circuit cavity QED, as well as to nano-electromechanical systems.Comment: 11 pages; 2 figures adde

    Cooling a nanomechanical resonator with quantum back-action

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    Quantum mechanics demands that the act of measurement must affect the measured object. When a linear amplifier is used to continuously monitor the position of an object, the Heisenberg uncertainty relationship requires that the object be driven by force impulses, called back-action. Here we measure the back-action of a superconducting single-electron transistor (SSET) on a radiofrequency nanomechanical resonator. The conductance of the SSET, which is capacitively coupled to the resonator, provides a sensitive probe of the latter's position;back-action effects manifest themselves as an effective thermal bath, the properties of which depend sensitively on SSET bias conditions. Surprisingly, when the SSET is biased near a transport resonance, we observe cooling of the nanomechanical mode from 550mK to 300mK-- an effect that is analogous to laser cooling in atomic physics. Our measurements have implications for nanomechanical readout of quantum information devices and the limits of ultrasensitive force microscopy (such as single-nuclear-spin magnetic resonance force microscopy). Furthermore, we anticipate the use of these backaction effects to prepare ultracold and quantum states of mechanical structures, which would not be accessible with existing technology.Comment: 28 pages, 7 figures; accepted for publication in Natur

    Quantum Theory of Cavity-Assisted Sideband Cooling of Mechanical Motion

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    We present a fully quantum theory describing the cooling of a cantilever coupled via radiation pressure to an illuminated optical cavity. Applying the quantum noise approach to the fluctuations of the radiation pressure force, we derive the opto-mechanical cooling rate and the minimum achievable phonon number. We find that reaching the quantum limit of arbitrarily small phonon numbers requires going into the good cavity (resolved phonon sideband) regime where the cavity linewidth is much smaller than the mechanical frequency and the corresponding cavity detuning. This is in contrast to the common assumption that the mechanical frequency and the cavity detuning should be comparable to the cavity damping.Comment: 5 pages, 2 figure

    Andreev bound states and Ο€\pi -junction transition in a superconductor / quantum-dot / superconductor system

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    We study Andreev bound states and Ο€\pi -junction transition in a superconductor / quantum-dot / superconductor (S-QD-S) system by Green function method. We derive an equation to describe the Andreev bound states in S-QD-S system, and provide a unified understanding of the Ο€\pi -junction transition caused by three different mechanisms: (1) {\it Zeeman splitting.} For QD with two spin levels E↑E_{\uparrow} and E↓E_{\downarrow}, we find that the surface of the Josephson current I(Ο•=Ο€2)I(\phi =\frac \pi 2) vs the configuration of (E↑,E↓)(E_{\uparrow},E_{\downarrow}) exhibits interesting profile: a sharp peak around E↑=E↓=0E_{\uparrow}=E_{\downarrow}=0; a positive ridge in the region of E↑⋅E↓>0E_{\uparrow}\cdot E_{\downarrow}>0; and a {\em % negative}, flat, shallow plain in the region of E↑⋅E↓<0E_{\uparrow}\cdot E_{\downarrow}<0. (2){\it \ Intra-dot interaction.} We deal with the intra-dot Coulomb interaction by Hartree-Fock approximation, and find that the system behaves as a Ο€\pi -junction when QD becomes a magnetic dot due to the interaction. The conditions for Ο€\pi -junction transition are also discussed. (3) {\it \ Non-equilibrium distribution.} We replace the Fermi distribution f(Ο‰)f(\omega) by a non-equilibrium one 12[f(Ο‰βˆ’Vc)+f(Ο‰+Vc)]\frac 12[ f(\omega -V_c)+f(\omega +V_c)] , and allow Zeeman splitting in QD where % E_{\uparrow}=-E_{\downarrow}=h. The curves of I(Ο•=Ο€2)I(\phi =\frac \pi 2) vs % V_c show the novel effect of interplay of non-equilibrium distribution with magnetization in QD.Comment: 18 pages, 8 figures, Late

    Quantum Noise Interference and Back-action Cooling in Cavity Nanomechanics

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    We present a theoretical analysis of a novel cavity electromechanical system where a mechanical resonator directly modulates the damping rate kappa of a driven electromagnetic cavity. We show that via a destructive interference of quantum noise, the driven cavity can effectively act like a zero-temperature bath irrespective of the ratio kappa / omega_M, where omega_M is the mechanical frequency. This scheme thus allows one to cool the mechanical resonator to its ground state without requiring the cavity to be in the so-called `good cavity' limit kappa << omega_M.Comment: 4+ pages, 2 figures. Error in second last paragraph correcte
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