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Bulletin of the American Physical Society

Quantum dynamics for a dissipative quantum harmonic oscillator as a model for a NEMS frequency control resonator

Ilki Kim, GERALD J. IAFRATE

Published Mar 16, 2006• 0 citations
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Classical decoherence in a nanomechanical resonator

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Decoherence is an essential mechanism that defines the boundary between classical and quantum behaviours, while imposing technological bounds for quantum devices. Little is known about quantum coherence of mechanical systems, as opposed to electromagnetic degrees of freedom. But decoherence can also be thought of in a purely classical context, as the loss of phase coherence in the classical phase space. Indeed the bridge between quantum and classical physics is under intense investigation, using, in particular, classical nanomechanical analogues of quantum phenomena. In the present work, by separating pure dephasing from dissipation, we quantitatively model the classical decoherence of a mechanical resonator: through the experimental control of frequency fluctuations, we engineer artificial dephasing. Building on the fruitful analogy introduced between spins/quantum bits and nanomechanical modes, we report on the methods available to define pure dephasing in these systems, while demonstrating the intrinsic almost-ideal properties of silicon nitride beams. These experimental and theoretical results, at the boundary between classical nanomechanics and quantum information fields, are prerequisite in the understanding of decoherence processes in mechanical devices, both classical and quantum. Introduction and background. Frequency noise in nano-mechanical systems (NEMS) is a topic intensely studied these last years, for both fundamental and practical reasons (references [ 13 – 23 ] of the paper): the frequency fluctuations can have an intrinsic origin linked to essential material properties, but they also limit the resolution of actual devices used as sensors. Recently, the Delft group proposed to analyze the effects of this noise on the dynamics of NEMS within a framework analogous to one of Nuclear Magnetic Resonance (NMR), or quantum bits (2014 Nat. Commun. 5 5819 ). Main results. Building on the analogy, in this paper we engineer frequency noise to study its impact on nano-resonators. We present a model experiment, with the full theory enabling the fit of data without free parameters. The effect of frequency noise is analogous to 'pure dephasing' in quantum bits, even though the device is a classical harmonic oscillator. As such, the analogy is very informative and interrogates the crossover between classical and quantum physics; it enters the class of 'classical analogues of quantum phenomena' studied in recent model nano-mechanical experiments (e.g. reference [ 10 ]). Wider implications. This is a broad topic that is of interest to many areas of science, far beyond NEMS and NMR. For the focused audience, we present the methods to quantitatively describe this 'classical pure dephasing' of NEMS, which can be used e.g. with carbon-based systems. As a conclusion, our results are a new tool for the understanding of classical decoherence in nano-resonators, and a pre-requisite for future experiments on quantum NEMS.

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We propose an approximation scheme to describe the dynamics of the spin-boson model when the spectral density of the environment shows a peak at a characteristic frequency $Ω$ which can be very close (or even equal) to the spin Zeeman frequency $Δ$. Mapping the problem onto a two-state system (TSS) coupled to a harmonic oscillator (HO) with frequency $ω_0$ we show that the representation of displaced HO states provides an appropriate basis to truncate the Hilbert space of the TSS-HO system and therefore a better picture of the system dynamics. We derive an effective Hamiltonian for the TSS-HO system, and show it furnishes a very good approximation for the system dynamics even when its two subsystems are moderately coupled. Finally, assuming the regime of weak HO-bath coupling and low temperatures, we are able to analytically evaluate the dissipative TSS dynamics.

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Decoherence is an essential mechanism that defines the boundary between classical and quantum behaviours, while imposing technological bounds for quantum devices. Little is known about quantum coherence of mechanical systems, as opposed to electromagnetic degrees of freedom. But decoherence can also be thought of in a purely classical context, as the loss of phase coherence in the classical phase space. Indeed the bridge between quantum and classical physics is under intense investigation, using, in particular, classical nanomechanical analogues of quantum phenomena. In the present work, by separating pure dephasing from dissipation, we quantitatively model the classical decoherence of a mechanical resonator: through the experimental control of frequency fluctuations, we engineer artificial dephasing. Building on the fruitful analogy introduced between spins/quantum bits and nanomechanical modes, we report on the methods available to define pure dephasing in these systems, while demonstrating the intrinsic almost-ideal properties of silicon nitride beams. These experimental and theoretical results, at the boundary between classical nanomechanics and quantum information fields, are prerequisite in the understanding of decoherence processes in mechanical devices, both classical and quantum. Introduction and background. Frequency noise in nano-mechanical systems (NEMS) is a topic intensely studied these last years, for both fundamental and practical reasons (references [ 13 – 23 ] of the paper): the frequency fluctuations can have an intrinsic origin linked to essential material properties, but they also limit the resolution of actual devices used as sensors. Recently, the Delft group proposed to analyze the effects of this noise on the dynamics of NEMS within a framework analogous to one of Nuclear Magnetic Resonance (NMR), or quantum bits (2014 Nat. Commun. 5 5819 ). Main results. Building on the analogy, in this paper we engineer frequency noise to study its impact on nano-resonators. We present a model experiment, with the full theory enabling the fit of data without free parameters. The effect of frequency noise is analogous to 'pure dephasing' in quantum bits, even though the device is a classical harmonic oscillator. As such, the analogy is very informative and interrogates the crossover between classical and quantum physics; it enters the class of 'classical analogues of quantum phenomena' studied in recent model nano-mechanical experiments (e.g. reference [ 10 ]). Wider implications. This is a broad topic that is of interest to many areas of science, far beyond NEMS and NMR. For the focused audience, we present the methods to quantitatively describe this 'classical pure dephasing' of NEMS, which can be used e.g. with carbon-based systems. As a conclusion, our results are a new tool for the understanding of classical decoherence in nano-resonators, and a pre-requisite for future experiments on quantum NEMS.
We study the entangling power of a nanoelectromechanical system (NEMS) simultaneously interacting with two separately trapped ions. To highlight this entangling capability, we consider a special regime where the ion-ion coupling does not generate entanglement in the system and any resulting entanglement will be the result of the NEMS acting as an entangling device. We study the dynamical behavior of the bipartite NEMS-induced ion-ion entanglement as well as the tripartite entanglement of the whole system (ions+NEMS\text{ions}+\text{NEMS}ions+NEMS). We found some quite remarkable phenomena in this hybrid system. For instance, the two trapped ions initially uncorrelated and prepared in coherent states can become entangled by interacting with a nanoelectromechanical resonator (also prepared in a coherent state) as soon as the ion-NEMS coupling achieves a certain value, and this can be controlled by external voltage gate on the NEMS device. We also show that, dynamically, the tripartite entanglement presents a more pronounced robustness against the destructive effects of dissipation when compared to the bipartite content.
We propose an approximation scheme to describe the dynamics of the spin-boson model when the spectral density of the environment shows a peak at a characteristic frequency ΩΩΩ which can be very close (or even equal) to the spin Zeeman frequency ΔΔΔ. Mapping the problem onto a two-state system (TSS) coupled to a harmonic oscillator (HO) with frequency ω0ω_0ω0​ we show that the representation of displaced HO states provides an appropriate basis to truncate the Hilbert space of the TSS-HO system and therefore a better picture of the system dynamics. We derive an effective Hamiltonian for the TSS-HO system, and show it furnishes a very good approximation for the system dynamics even when its two subsystems are moderately coupled. Finally, assuming the regime of weak HO-bath coupling and low temperatures, we are able to analytically evaluate the dissipative TSS dynamics.