2000
DOI: 10.1126/science.287.5452.463
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Information Storage and Retrieval Through Quantum Phase

Abstract: Information was stored as quantum phase in an N-state Rydberg atom data register. One or more flipped states stored in an eight-state atomic wave packet could be retrieved in a single operation, in agreement with a recent proposal by Grover.Storage of information as quantum phase was first proposed several years ago in connection with a new class of computational algorithms based on the rules of quantum mechanics rather than classical physics (1). The analog of the binary bit, which is the smallest piece of cl… Show more

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Cited by 274 publications
(174 citation statements)
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“…This remains true even if the generic fluctuations of the ionization rate (see section 7.1) may induce locally (in some control parameter) large deviations between individual 3D and 1D decay rates 35 . Therefore, the transition from dominant ionization to dominant spontaneous decay will shift to slightly higher values of n 0 in 3D.…”
Section: Linearly Polarized Microwavementioning
confidence: 99%
See 1 more Smart Citation
“…This remains true even if the generic fluctuations of the ionization rate (see section 7.1) may induce locally (in some control parameter) large deviations between individual 3D and 1D decay rates 35 . Therefore, the transition from dominant ionization to dominant spontaneous decay will shift to slightly higher values of n 0 in 3D.…”
Section: Linearly Polarized Microwavementioning
confidence: 99%
“…Apart from their possible practical applications (for example, for the purpose of quantum control of atomic or molecular fragmentation processes [28], or for information storage [35][36][37][38] in a confined volume of (phase) space for long times), they show the fruitful character of classical nonlinear dynamics. Indeed, here the nonlinearity is not a nuisance to be minimized, but rather the essential ingredient.…”
Section: The Interest Of Non-dispersive Wave-packetsmentioning
confidence: 99%
“…Among examples are: all optical interferometry, 21,22 cavity quantum electrodynamics, 23 ion traps, 24 superconducting Josephson junctions, 25 and an explosion of studies in NMR following the initial propositions. 26,27 More specific tasks, such as a search algorithm through the preparation and manipulation of Rydberg Superposition states in atomic beams, 28 have also been demonstrated. The latter belongs to the category that does not require entanglement, 29 and therefore can be argued that does not allow exponential speed-up without the expenditure of an exponential overhead in resources.…”
Section: Introductionmentioning
confidence: 99%
“…In the case of neutral atoms, the requirement that the gate operation time is short compared to the typical time of decoherence mechanisms, including spontaneous emission, collisions, ionization of the Rydberg states, transitions induced by black body radiation, or motional excitation of the atoms trapped in an optical lattice, leads to the search of state-selective Rydberg excitation schemes using femtosecond pulses. Despite the fact that excitation to a single n-Rydberg level requires nanosecond or cw lasers with a narrow bandwidth, coherent control tools as control algorithms to optimally shape femtosecond laser pulses have been successfully used to address a single transition [6,7], as well as multipulse schemes using 150 fs pulses, which alone would populate about ten n-Rydberg levels, have shown the ability to selectively populate a single or a few levels [8,9]. These different schemes address the excitation of relatively high Rydberg levels, typically of principal quantum numbers as n ∼ 30.…”
Section: Introductionmentioning
confidence: 99%