2022
DOI: 10.1103/physrevapplied.17.034020
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Force Sensing in an Optomechanical System with Feedback-Controlled In-Loop Light

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Cited by 22 publications
(11 citation statements)
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“…Furthermore, this hybrid optomechanical system contains an ensemble of N number of two-level ultracold atoms trapped inside it and interacts non-resonantly with the intracavity field and a classical control field. For a sufficiently large value of N, this trapped atomic ensemble behaves effectively as a negative-mass oscillator (NMO) [92,93,[96][97][98][99]. The cavity mode is also coherently driven by a classical field of frequency, ω L ,; input power, P L ; and wavelength, λ L .…”
Section: The Model Hamiltonianmentioning
confidence: 99%
“…Furthermore, this hybrid optomechanical system contains an ensemble of N number of two-level ultracold atoms trapped inside it and interacts non-resonantly with the intracavity field and a classical control field. For a sufficiently large value of N, this trapped atomic ensemble behaves effectively as a negative-mass oscillator (NMO) [92,93,[96][97][98][99]. The cavity mode is also coherently driven by a classical field of frequency, ω L ,; input power, P L ; and wavelength, λ L .…”
Section: The Model Hamiltonianmentioning
confidence: 99%
“…A variety of experiments explore mechanical resonators of different masses and sizes. The properties of these systems and their ability to interact with external systems allow conceptually different applications ranging from gravitational wave sensing [3], compact sensors of various external stimuli [4][5][6][7][8], and stochastic heat engines [9][10][11][12], to quantum mechanical entanglement [13][14][15] or photon-phonon transducers in quantum networks [16][17][18].…”
Section: Introductionmentioning
confidence: 99%
“…The vibrational modes supported by a structure can be complex, depending on the structure's geometry, and can be fundamentally understood in the context of the theory of elasticity to form a collection of normal modes. This multimodeness can be a limitation in feedback cooling experiments where the signal of an optical mode whose phase is sensitive to mechanical motion is used to produce a negative feedback on the oscillator to damp its motion [8,20,[34][35][36][37]. Likewise, besides specific advantageous situations where the ratio of mechanical modes' frequencies is integer [23], it limits the ability of a pulsed position measurement to estimate one quadrature of a single mechanical resonator while evading backaction, as any instantaneous measurement probes all modes at once [21,22].…”
Section: Introductionmentioning
confidence: 99%
“…Quantum optical interferometers exploit the interference between a probe and a reference beam to detect weak signals [10], a prominent example being the detection of gravitational waves from black hole mergers [11,12]. A similar approach can be adopted for microwave traveling waves [13], microwave cavity fields [14], matter waves [15,16], between light and atomic ensembles [17,18], and optomechanics [19][20][21].…”
Section: Introductionmentioning
confidence: 99%
“…Quantum optical interferometers exploit the interference between a probe and a reference beam to detect weak signals [10], a prominent example being the detection of gravitational waves from black hole mergers [11,12]. A similar approach can be adopted for microwave traveling waves [13], microwave cavity fields [14], matter waves [15,16], between light and atomic ensembles [17,18], and optomechanics [19][20][21].Numerous sensing proposals use quantum non-Gaussian states as probes for improved estimation of phase and displacement [22][23][24]. For example, quantum displacement sensing has been performed with Fock states and non-Gaussian superpositions of Fock states of the phononic modes of trapped ions [25,26].…”
mentioning
confidence: 99%