Mechanical oscillator thermometry in the nonlinear optomechanical regime
- URL: http://arxiv.org/abs/2006.06699v1
- Date: Thu, 11 Jun 2020 18:00:04 GMT
- Title: Mechanical oscillator thermometry in the nonlinear optomechanical regime
- Authors: Victor Montenegro, Marco G. Genoni, Abolfazl Bayat, Matteo G. A. Paris
- Abstract summary: We study an undriven optomechanical system via non-Gaussian radiation-pressure interaction.
We show that the optical probe gets a nonlinear phase, resulting from the non-Gaussian interaction, and undergoes an incoherent phase diffusion process.
To efficiently infer the temperature from the entangled light-matter state, we propose using a nonlinear Kerr medium before a homodyne detector.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: Optomechanical systems are promising platforms for controlled light-matter
interactions. They are capable of providing several fundamental and practical
novel features when the mechanical oscillator is cooled down to nearly reach
its ground state. In this framework, measuring the effective temperature of the
oscillator is perhaps the most relevant step in the characterization of those
systems. In conventional schemes, the cavity is driven strongly, and the
overall system is well-described by a linear (Gaussian preserving) Hamiltonian.
Here, we depart from this regime by considering an undriven optomechanical
system via non-Gaussian radiation-pressure interaction. To measure the
temperature of the mechanical oscillator, initially in a thermal state, we use
light as a probe to coherently interact with it and create an entangled state.
We show that the optical probe gets a nonlinear phase, resulting from the
non-Gaussian interaction, and undergoes an incoherent phase diffusion process.
To efficiently infer the temperature from the entangled light-matter state, we
propose using a nonlinear Kerr medium before a homodyne detector. Remarkably,
placing the Kerr medium enhances the precision to nearly saturate the ultimate
quantum bound given by the quantum Fisher information. Furthermore, it also
simplifies the thermometry procedure as it makes the choice of the homodyne
local phase independent of the temperature, which avoids the need for adaptive
sensing protocols.
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