2011
DOI: 10.1103/physrevlett.107.083601
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Quantum Metrology with Entangled Coherent States

Abstract: We present an improved phase estimation scheme employing entangled coherent states and demonstrate that these states give the smallest variance in the phase parameter in comparison to NOON, "bat," and "optimal" states under perfect and lossy conditions. As these advantages emerge for very modest particle numbers, the optical version of entangled coherent state metrology is achievable with current technology.

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Cited by 463 publications
(257 citation statements)
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“…[104][105][106][107][108][109] In parallel, studies on how to use quantum phenomena in metrology and sensing emerged, aiming to reach sensitivities beyond the limit imposed by classical physics. [110,111] While discussions continue on the ultimate limit of quantum sensing, [112][113][114][115][116] the use of single-electron spins Figure 4. SEM image of the single phosphorus spin qubit device developed at UNSW.…”
Section: Diamond Quantum Sensingmentioning
confidence: 99%
“…[104][105][106][107][108][109] In parallel, studies on how to use quantum phenomena in metrology and sensing emerged, aiming to reach sensitivities beyond the limit imposed by classical physics. [110,111] While discussions continue on the ultimate limit of quantum sensing, [112][113][114][115][116] the use of single-electron spins Figure 4. SEM image of the single phosphorus spin qubit device developed at UNSW.…”
Section: Diamond Quantum Sensingmentioning
confidence: 99%
“…The quantum Fisher information (QFI), which quantifies a state's ability to measure a phase φ, for a general density matrix ρ, is given by [32][33][34] …”
Section: No Loss: Superposition States Are Sufficientmentioning
confidence: 99%
“…Our analysis is in good agreement with the experimental results. This method may enable the continuous deterministic entanglement of two light beams for measurements below the standard quantum limit [27,28], the nondestructive detection of individual photons by measuring cavity reflection instead of transmission [22], the imprinting of large photon-photon phase shifts [1,29] by conducting the same experiment away from atomic resonance, and the production of polarization entangled states by extension to another internal state [30,31]. The experimental system [14] is shown in Fig.…”
mentioning
confidence: 99%