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Dynamics of some single flux quantum devices: I. Parametric quantron
116
Citations
6
References
1977
Year
EngineeringCavity QedI. Parametric QuantronJosephson JunctionsQuantum LogicQuantum ComputingQuantum SystemsQuantum ControlQuantum MatterJosephson GateQuantum ElectronicsQuantum SciencePhysicsQuantum DeviceQuantum InformationComputer EngineeringQuantum SwitchesParametric QuantronQuantum TransducersQuantum TechnologySingle Flux QuantaNatural SciencesCondensed Matter PhysicsApplied PhysicsQuantum DevicesQuantum Hardware
In this paper and the following one, the properties of two systems operating with single flux quanta are calculated. The first system is a quantron (a one-junction interferometer) with a Josephson gate as a junction. By a proper change of its critical current in time, the switching of quantron stable states can be controlled by a small external flux much less than Φ <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">o</inf> . This "Parametric Quantron" can be used as the basic cell of a Single Quantum Logic System. The most wonderful property of this device is that the energy dissipation during one logical step (PτT factor) can be much less than the thermal energy K <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">B</inf> T and is limited by quantum effects only: Pτ <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> \simg10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> h.
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