Abstract

Realizing quantum mechanical behavior in micro- and nanomechanical resonators has attracted continuous research effort. One of the ways for observing quantum nature of mechanical objects is via the mechanism of phonon blockade. Here, we show that phonon blockade could be achieved in a system of two weakly nonlinear mechanical resonators coupled by a Coulomb interaction. The optimal blockade arises as a result of the destructive quantum interference between paths leading to two-phonon excitation. It is observed that, in comparison to a single drive applied on one mechanical resonator, driving both the resonators can be beneficial in many aspects; such as, in terms of the temperature sensitivity of phonon blockade and also with regard to the tunability, by controlling the amplitude and the phase of the second drive externally. We also show that via a radiation pressure induced coupling in an optomechanical cavity, phonon correlations can be measured indirectly in terms of photon correlations of the cavity mode.

Highlights

  • Reaching the quantum regime of micro- and nanomechanical resonators has significance in weak force detection1,2 as well as quantum information processing3–5

  • Different from this, here we show that phonon blockade in a weakly nonlinear mechanical resonator can be realized by coupling it to another weakly nonlinear mechanical resonator via Coulomb interaction37–39

  • Phonon correlations are characterised in terms of the second-order correlation function

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Summary

Introduction

Reaching the quantum regime of micro- and nanomechanical resonators has significance in weak force detection1,2 as well as quantum information processing3–5. Conventional phonon blockade has been studied in a mechanical resonator with a Kerr-type nonlinearity36. In the case of single drive, we show that under optimal conditions for the detuning, Δ, and Kerr nonlinearity, U, phonon blockade could be achieved.

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