2007
DOI: 10.1103/physreva.76.031806
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High-photon-number path entanglement in the interference of spontaneously down-converted photon pairs with coherent laser light

Abstract: We show that the quantum interference between down-converted photon pairs and photons from coherent laser light can produce a maximally path entangled N-photon output component with a fidelity greater than 90% for arbitrarily high photon numbers. A simple beam splitter operation can thus transform the two-photon coherence of down-converted light into an almost optimal N-photon coherence.

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Cited by 100 publications
(105 citation statements)
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“…A post-selected proof of principle experiment that employs some of these optimal states was recently performed [66]. Note that, for very low values of loss, NOON states retain their optimality [104,106], and can be approximated by states that are easy to generate [67,68]. Also, a very simple proposal based on parametric downconversion which can be realized without post-selection was proposed in [72]: it can achieve the Heisenberg bound for low loss and degrades gracefully with noise.…”
Section: Quantum Metrology With Noisementioning
confidence: 99%
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“…A post-selected proof of principle experiment that employs some of these optimal states was recently performed [66]. Note that, for very low values of loss, NOON states retain their optimality [104,106], and can be approximated by states that are easy to generate [67,68]. Also, a very simple proposal based on parametric downconversion which can be realized without post-selection was proposed in [72]: it can achieve the Heisenberg bound for low loss and degrades gracefully with noise.…”
Section: Quantum Metrology With Noisementioning
confidence: 99%
“…This is possible via some rather complicated optical schemes [57][58][59][60][61] which have only been implemented in highly refined, but post-selected experiments [61][62][63][64][65][66]. However states which possess a high fidelity with the NOON states, also for large values of N , can be simply obtained by mixing a squeezed vacuum and a coherent state at a beam splitter [67][68][69]. Introducing such states at the input of a Mach-Zehnder, a scaling N −1 in the average photon number of photons employed in a given experimental run can be achieved [1].…”
Section: Applications In Quantum Interferometrymentioning
confidence: 99%
“…1(a)], the probability of detecting all of the photons at a given position will display spatial fringes with a period of λ=ð2N sinðθ=2ÞÞ, where θ is the angle betweenk 1 andk 2 (assuming jk 1 j ¼ jk 2 j ¼ ð2π=λÞ). The period of the N00N fringes is N times smaller than that of classical fringes, suggesting that N00N states could be used to increase the resolution of optical systems by a factor of N. This observation has led to much subsequent work on N00N states [4,5,[13][14][15][16] and their application in tasks such as quantum lithography and quantum imaging [10][11][12]17]. However, the individual photons in the N00N state cannot be localized to better than λ=2, regardless of the narrow spatial scale of the N-photon correlation fringes [6,7].…”
mentioning
confidence: 99%
“…To generate N00N states, the relative phase between the two arms must be set to zero, and the relative amplitudes balanced. The source is optimized for N00N states of different N by simply changing the relative amplitude between the laser and DC light [15]. Ideally, two-and three-photon N00N states can be made perfectly by setting the two-photon rate from the laser equal to that from the DC light (which we will refer to as "configuration 1").…”
Section: Prl 112 223602 (2014) P H Y S I C a L R E V I E W L E T T Ementioning
confidence: 99%
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