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Andreev reflection, named after the Russian physicist Alexander F. Andreev, is a type of particle scattering which occurs at interfaces between a superconductor (S) and a normal state material (N). It is a charge-transfer process by which normal current in N is converted to supercurrent in S.
The superconducting gap can be induced using Andreev reflection, by putting the wire in the proximity to a superconductor. [8] [9] Realizations using 3D topological insulators have also been proposed. [9] There is no single definitive way to test for Majorana zero modes.
These materials are type-II superconductors with substantial upper critical field H c2, and in contrast to, for example, the cuprate superconductors with even higher H c2, they can be easily machined into wires. Recently, however, 2nd generation superconducting tapes are allowing replacement of cheaper niobium-based wires with much more ...
Conversely, the (gapless) electron order present in the normal metal is also carried over to the superconductor in that the superconducting gap is lowered near the interface. The microscopic model describing this behavior in terms of single electron processes is called Andreev reflection. It describes how electrons in one material take on the ...
Assume that superconductor A has Ginzburg–Landau order parameter =, and superconductor B =, which can be interpreted as the wave functions of Cooper pairs in the two superconductors. If the electric potential difference across the junction is V {\displaystyle V} , then the energy difference between the two superconductors is 2 e V ...
Calculated magnetization curve for a superconducting slab, based on Bean's model. The superconducting slab is initially at H = 0. Increasing H to critical field H* causes the blue curve; dropping H back to 0 and reversing direction to increase it to -H* causes the green curve; dropping H back to 0 again and increase H to H* causes the orange curve.
The most commonly used conventional superconductor in applications is a niobium-titanium alloy - this is a type-II superconductor with a superconducting critical temperature of 11 K. The highest critical temperature so far achieved in a conventional superconductor was 39 K (-234 °C) in magnesium diboride.
Design was theoretically described in 1997 by Shnirman, [11] while the evidence of quantum coherence of the charge in a Cooper pair box was published in February 1997 by Vincent Bouchiat et al. [12] In 1999, coherent oscillations in the charge Qubit were first observed by Nakamura et al. [13] Manipulation of the quantum states and full ...