A suspended carbon-nanotube resonator is modelled as a single mode of effective mass…

PHYSICS · Subjective · Fermi University Physics · Quantum Mechanics · Quantum dynamics and its formulations · Quantum dynamics and its formulations

The Structure of Quantum Mechanics, Ch Coherent states, Ehrenfest's theorem and the classical limit

Problem

A suspended carbon-nanotube resonator is modelled as a single mode of effective mass m=1.0×10−20 kgm=1.0\times10^{-20}\,\mathrm{kg} and angular frequency ω=2π×100 MHz\omega=2\pi\times100\,\mathrm{MHz}, undamped and at zero temperature. Its potential is not quite harmonic, V(x)=12mω2x2+λx4V(x)=\tfrac12m\omega^2x^2+\lambda x^4, with λ=mω2/2xD2\lambda=m\omega^2/2x_D^2 and xD=10 nmx_D=10\,\mathrm{nm}, the displacement at which the quartic term would equal the quadratic one. Classically, such an oscillator swinging with amplitude AA has angular frequency ω(A)=ω(1+3λA2/2mω2)\omega(A)=\omega\big(1+3\lambda A^2/2m\omega^2\big). The tube is prepared in a coherent state caught at rest at ⟨x^⟩=A=1.0 nm\langle\hat x\rangle=A=1.0\,\mathrm{nm} and then watched for 1.0 ms1.0\,\mathrm{ms}. (a) Find the width Δx\Delta x and the mean quantum number nˉ\bar n of the state, taking the width to be the harmonic ground-state width. (b) Evaluate the force ratio ∣V′′′(A)∣(Δx)2/∣V′(A)∣|V'''(A)|(\Delta x)^2/|V'(A)| and the action in units of ℏ\hbar, and say whether the force and action conditions are met. (c) A coherent state of amplitude AA has A2=2ℏnˉ/mωA^2=2\hbar\bar n/m\omega. Use this to turn ω(A)\omega(A) into a drift δω\delta\omega of the level spacing per level, then estimate tspreadt_{\rm spread} and compare it with the watching time. (d) Does the tube's motion have a trajectory over the 1 ms1\ \mathrm{ms} it is watched? Say which condition decides.

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