2021
DOI: 10.1103/physrevlett.127.233201
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Invariance Property of the Fisher Information in Scattering Media

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Cited by 4 publications
(3 citation statements)
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“…A related observation was subsequently also reported in Ref. 211 which numerically studied systems without any absorption: if the average dwell time is constant, so is the average precision with which a particle's property can be estimated, as long as the scattering regime is ballistic or diffusive (but not Anderson localized). The physics of the underlying RCA mechanisms extends of course to more complex tasks, such as the recognition of sub-wavelength object shapes or materials inside an RCA without any manipulation in the extreme proximity of the scene.…”
Section: B Meta-programmable Reverberation-coded Aperturessupporting
confidence: 53%
“…A related observation was subsequently also reported in Ref. 211 which numerically studied systems without any absorption: if the average dwell time is constant, so is the average precision with which a particle's property can be estimated, as long as the scattering regime is ballistic or diffusive (but not Anderson localized). The physics of the underlying RCA mechanisms extends of course to more complex tasks, such as the recognition of sub-wavelength object shapes or materials inside an RCA without any manipulation in the extreme proximity of the scene.…”
Section: B Meta-programmable Reverberation-coded Aperturessupporting
confidence: 53%
“…To acquire the information states, a great challenge lies in the random scattering caused by the disorder of complex systems, which causes signal attenuation and weakens the observable wave field features 15,16 . Over the years, many operators or matrices based on physical features of wave field properties have been derived, including transmission matrix engineering 17 , the energy deposition matrix 18 , the crosscorrelations operator 19 , the generalized Wigner-Smith (GWS) operator 20,21 , the Floquet scattering matrix 22 , the acousto-optical transmission matrix 23 , the deposition matrix 24 , the random matrix theory for the coherent perfect absorption 25,26 , and Fisher information operator 27 . They all provide useful mathematical tools for studying the interaction mechanism between wave field and scattering spaces.…”
Section: Introductionmentioning
confidence: 99%
“…To demonstrate our approach for constructing optimal tractor beam states, we first compute a unitary scattering matrix (for which the GWS operator is Hermitian, hence the eigenstate corresponding to the most positive eigenvalue then describes the input field of the optimal tractor beam). Since procedures for how to set up this scattering matrix in an appropriate basis (in free space) don't seem to be available in the literature, we present a comprehensive description of our solution in the following, with the details being available in Appendix A and the code being published alongside this work [39]. Restricting our analysis to two spatial dimensions, our starting point is the scalar Helmholtz equation in polar coordinates, [∆ + k 2 ε( r)]ψ( r) = 0, in a circular region (see Fig.…”
mentioning
confidence: 99%