2009
DOI: 10.1103/physreva.80.063811
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Metrological resolution and minimum uncertainty states in linear and nonlinear signal detection schemes

Abstract: We study the performance of linear and nonlinear optical schemes for the detection of weak signals for two classes of probe states. These are quadrature coherent squeezed states and the minimum uncertainty states of the generator of the transformation and the measured observable. Both for linear and nonlinear schemes we show that the generator-measurement minimum uncertainty states are far from being optimum, while the quadrature coherent squeezed states can reach maximum accuracy almost for the same amount of… Show more

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Cited by 16 publications
(20 citation statements)
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“…Several Authors [80][81][82][83][84][85][86][87][88][89][90][91][92][93][94][95][96] have recently considered the possibility of using nonlinear effects to go beyond the N −1 Heisenberg-like scalings in phase estimation problems. These new regimes have been called "superHeisenberg" scalings in Ref.…”
Section: Beyond the Heisenberg Bound: Nonlinear Estimation Strategiesmentioning
confidence: 99%
See 1 more Smart Citation
“…Several Authors [80][81][82][83][84][85][86][87][88][89][90][91][92][93][94][95][96] have recently considered the possibility of using nonlinear effects to go beyond the N −1 Heisenberg-like scalings in phase estimation problems. These new regimes have been called "superHeisenberg" scalings in Ref.…”
Section: Beyond the Heisenberg Bound: Nonlinear Estimation Strategiesmentioning
confidence: 99%
“…[97]. Ultimately the idea of these proposals is to consider settings where the unitary transformation that "writes" the unknown parameter x into the probing signals, is characterized by many-body Hamiltonian generators which are no longer extensive functions of the number of probes employed in the estimation [83][84][85][86][87][88][89][90][91][92] or, for the optical implementations which yielded the inequality (6), in the photon number operator of the input signals [80][81][82][83][93][94][95][96]. Consequently, in these setups, the mapping (e −ixH ) ⊗n which acts on the input states ρ (n) 0 , gets replaced by a transformations of the form e −ixH (n) which couples the probes non trivially.…”
Section: Beyond the Heisenberg Bound: Nonlinear Estimation Strategiesmentioning
confidence: 99%
“…Concerning nonlinear schemes, the most simple example in the single-mode case is G =n k . Variance scaling as G ∝ n k can be reached by quadrature squeezed states, while quadrature coherent states lead to G ∝ n k−1/2 [7,10,16].…”
Section: Unbounded Number Of Particlesmentioning
confidence: 99%
“…Typical effective generators for light propagation in nonresonant nonlinear media are given by powers and products of photon-number operators of the form G =n k in a single-mode approach [4,5,7,8,16,24], G = J 2 z in a two-mode scheme [4], G = ⊗ k jn j in a multimode configuration [7], or even G = jn k j [23].…”
Section: Nonlinear Opticsmentioning
confidence: 99%
“…(2.10). However, this is not quite so optimum strategy since some other probes may lead to smaller φ via a larger G even though they are not minimum [25].…”
Section: Simple Estimationmentioning
confidence: 99%