2006
DOI: 10.1103/physreva.74.013808
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Generation of a highly-phase-sensitive polarization-squeezedN-photon state by collinear parametric down-conversion and coherent photon subtraction

Abstract: We propose a new type of a Heisenberg-limited quantum interferometer, whose input is indistinguishably photon-subtracted twin beams. Such an interferometer can yield Heisenberg-limited performance while at the same time giving a direct fringe reading, unlike for the twin-beam input of the Holland-Burnett interferometer. We propose a feasible experimental realization, using a nondegenerate optical parametric oscillator above threshold.

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Cited by 11 publications
(8 citation statements)
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References 45 publications
(71 reference statements)
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“…path-entangled n-photon states, such as NOON states [6,7] or other non-classical states [8,9,10,11,12,13,14]. However, such states are very difficult to produce experimentally even for moderate n [15,16,17,18,19,20,21,22].…”
Section: Introductionmentioning
confidence: 99%
“…path-entangled n-photon states, such as NOON states [6,7] or other non-classical states [8,9,10,11,12,13,14]. However, such states are very difficult to produce experimentally even for moderate n [15,16,17,18,19,20,21,22].…”
Section: Introductionmentioning
confidence: 99%
“…It is worth mentioning that states like |ψ ± have been shown to achieve Heisenberg-limit of phase measurements in quantum interferometry [55,56]. We now consider a third PNR detector placed in the path of mode 'b' to detect n 3 photons.…”
Section: Proposed Method: Analytical Modelmentioning
confidence: 99%
“…S(z) ab = e zâ † b † −z * âb (54) (55) where r = cos θ is the beamsplitter reflection coefficient and z = Re iπ is the complex squeezing parameter. After applying the squeezing operation to vacuum and sending the two modes a and b through beamsplitters, PNR detection is performed using the POVM for a lossy PNR detector detector, which is given as…”
Section: Appendix a Numerical Modelingmentioning
confidence: 99%
“…where the sum is taken over even values of N. If we postselect N photons from this state, the state is equivalent to the Holland-Burnett state ñ |N N 2, 2 HV [13]. To generate the Yurke state [35], one photon is subtracted from the down-converted photon source, by detection of a single-photon in the D/A basis. After the one-photon subtraction, the conditional output is the five-photon Yurke state.…”
Section: Methodsmentioning
confidence: 99%
“…We report on an optical implementation of a spin-squeezing model which was originally considered by Yurke et al [33,34], and we investigate how sensitivity is improved in this model. Our setup generates five-photon Yurke states by postselecting on cases with five detection events from the state emitted by a parametric downconversion source after one photon subtraction [35], and we use spatially-multiplexed pseudo-number-resolving detection to reconstruct photon-number statistics at the output [15]. Our analysis demonstrates increased sensitivity from the observed optical Yurke state, using all five-photon coincidence outcomes.…”
Section: Introductionmentioning
confidence: 99%