Titlebook: Single Charge Tunneling; Coulomb Blockade Phe Hermann Grabert,Michel H. Devoret Book 1992 Springer Science+Business Media New York 1992 Cou

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勉强

Josephson Effect in Low-Capacitance Tunnel Junctions,ies are the Josephson energy . ., the charging energy . . = . ./2., and the thermal energy . . .. Equally important are the characteristic resistances: the normal state resistance . ., the quantum resistance. . . = . . = 6453 Ω, and the impedance of free space . . = 377 Ω. The fact that . . ≪ . impl

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Coulomb-Blockade Oscillations in Semiconductor Nanostructures,see Fig. 1) [1]–[5]. The conductance oscillations occur as the voltage on a nearby gate electrode is varied. This setup is the SET transistor described in Sec. 6 of Chap. 2. The number . of conduction electrons on an island (or dot) between two tunnel barriers is an integer, so that the charge . = —

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One-Dimensional Arrays of Small Tunnel Junctions,upled arrays of many, closely spaced, ultrasmall junctions. For example, the time correlation of tunnel events was first observed in such an array. The interpretation of the results obtained with an array may be complicated as compared to a single junction, but the additional degrees of freedom for

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Possible Applications of the Single Charge Tunneling,he reason is that the present-day applied physics literature is full of descriptions of various electronic “devices” which have no real chance to be used in practice, because their possible performance is inferior to that of commercially available devices. (Most amusing is that in most cases this co

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Book 1992ir, leads to macro­ scopically observable effects. The first conference entirely devoted to this new field was the NATO Advanced Study Institute on Single Charge Tunneling held in Les Hauches, France, March 5-15, 1991. This book contains a series of tutorial articles based on lectures presented at t

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Introduction to Single Charge Tunneling,lectrons are traversing the insulating gaps one at a time. Nevertheless, the successive tunnel events across a particular junction are uncorrelated and constitute a Poisson process. The key point is that, during its journey from the source to the drain, the electron necessarily makes the charge of the island vary by ..

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