2005
DOI: 10.1364/josab.22.000499
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Experimental realization of a quantum quincunx by use of linear optical elements

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Cited by 126 publications
(125 citation statements)
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“…Here unitary coin operator C and the conditioned shift operator S for QRW are given by the Eqs. (8) and (9) of the previous section.…”
Section: Qrw Of Two Photons With Separable Initial Statementioning
confidence: 92%
See 1 more Smart Citation
“…Here unitary coin operator C and the conditioned shift operator S for QRW are given by the Eqs. (8) and (9) of the previous section.…”
Section: Qrw Of Two Photons With Separable Initial Statementioning
confidence: 92%
“…As a result various classical sources like low intensity lasers [8,13] and coherent state of radiation fields [4,14] are used to realize QRW. In order to explore further the quantum nature of random walk, we consider the case when two photons start QRW from a separable initial state…”
Section: Qrw Of Two Photons With Separable Initial Statementioning
confidence: 99%
“…Single photon detector posed linear-optical version of the Galton board based on beamsplitters and phaseshifters [12,27]. A similar, polarization-encoded setup has been proposed for cube polarizing beamsplitters [28].…”
Section: Pbsmentioning
confidence: 99%
“…3 These properties generated broad interest in applying QWs to quantum information processing tasks. 4 Experimentally, QWs have been implemented using a wide array of platforms, including photonics, [5][6][7][8][9][10][11][12] trapped ions, 13,14 and ultra-cold atoms. [15][16][17] The current degree of experimental control of these systems is remarkable: it is possible to prepare an initial state with single-site and single-particle resolution, to control almost every aspect of the lattice potential, and to directly monitor the evolving wave function.…”
Section: Introductionmentioning
confidence: 99%
“…[15][16][17] The current degree of experimental control of these systems is remarkable: it is possible to prepare an initial state with single-site and single-particle resolution, to control almost every aspect of the lattice potential, and to directly monitor the evolving wave function. Early experiments demonstrated the behavior of single-particle QWs; however, these dynamics can be desribed by classical wave equations (indeed, some of these experiments were performed with coherent light) [5][6][7]9 ), and thus cannot display non-classical features. Non-classical behavior can be observed when several indistinguishable particles participate in the QW simultaneously, as was shown both theoretically 7,12,[18][19][20] and experimentally.…”
Section: Introductionmentioning
confidence: 99%