2021
DOI: 10.1103/physreva.103.013710
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Generation of optical Schrödinger cat states by generalized photon subtraction

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Cited by 61 publications
(50 citation statements)
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“…This advantage for m=0 with respect to two‐mode squeezed vacuum can be attributed to the single‐mode squeezing required in the generation of Schrödinger cat state (ref. [77] and references therein) which are used for preparing superposed bipartite coherent states at a beam‐splitter. [ 78 ] However, false|ψfalse⟩ has similar advantage only after considerable number of photon addition, that is, m2.…”
Section: Teleportation Of a Single‐mode Statementioning
confidence: 99%
“…This advantage for m=0 with respect to two‐mode squeezed vacuum can be attributed to the single‐mode squeezing required in the generation of Schrödinger cat state (ref. [77] and references therein) which are used for preparing superposed bipartite coherent states at a beam‐splitter. [ 78 ] However, false|ψfalse⟩ has similar advantage only after considerable number of photon addition, that is, m2.…”
Section: Teleportation Of a Single‐mode Statementioning
confidence: 99%
“…In particular, let = 0 . If we measure the first output channel and detect m photons, then the unnormalized reduced density matrix is Remark 16 Many schemes like those proposed in [87][88][89][90][91][92][93][94][95][96] that generate Schrödinger cat states can be described uniformly in the mathematical framework similar to that discussed above.…”
Section: Schrödinger Cat States Generationmentioning
confidence: 99%
“…These states have been produced experimentally using the optical Kerr effect in 1986 by Yurke and Stoler [8]. Among more recent experimental procedures suggested for generation of optical cat states are the method based on photon subtraction of an optical squeezed state [9][10][11][12] and the protocol that uses homodyne detection and photon number states [13] (see [14] for a review on generating cat states).…”
Section: Introductionmentioning
confidence: 99%