By A. A. Varlamov (auth.), Anatolie Sidorenko (eds.)
This e-book demonstrates how the recent phenomena in superconductivity at the nanometer scale (FFLO country, triplet superconductivity, Crossed Andreev mirrored image, synchronized iteration etc.) function the foundation for the discovery and improvement of novel nanoelectronic units and structures. It demonstrates how quite complicated principles and theoretical versions, like odd-pairing, non-uniform superconducting nation, pi-shift etc., correctly describe the techniques in genuine superconducting nanostructues and novel units according to them. The booklet turns out to be useful for a vast viewers of readers, researchers, engineers, PhD-students, lectures and others who wish to achieve wisdom within the frontiers of superconductivity on the nanoscale.
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Extra resources for Fundamentals of Superconducting Nanoelectronics
Lett. 89, 287001 (2002) 27. A. Levchenko, M. A. Varlamov, Phys. Rev. B 83, 020506 (R) (2011) 28. A. Varlamov, A. Kavokin, Europhys. Lett. 87, 47007 (2009) 29. A. Abrikosov, Fundamentals of the Theory of Metals (North Holland, 1988) 30. Hereafter „ D kB D c D 1 31. For simplicity in this subsection the magnetic field is assumed to be zero 32. V.
Huse, Phys. Rev. Lett. 89, 287001 (2002) 27. A. Levchenko, M. A. Varlamov, Phys. Rev. B 83, 020506 (R) (2011) 28. A. Varlamov, A. Kavokin, Europhys. Lett. 87, 47007 (2009) 29. A. Abrikosov, Fundamentals of the Theory of Metals (North Holland, 1988) 30. Hereafter „ D kB D c D 1 31. For simplicity in this subsection the magnetic field is assumed to be zero 32. V.
80) can also be obtained also from the uncertainty principle. T Tc0 /, as was done in the vicinity of Tc0 . The spatial coherence scale QF e h can be estimated from the value of QF analogously to consideration near Tc0 . Namely, two electrons with the coherent phase starting from the same point after the time QF get separated by the distance QF Á e h D 1=2 QF BCS = p e h: To clarify the physical meaning of QF and QF , note that near the quantum phase transition at zero temperature, where H ! r; t/ become highly inhomogeneous, contrary to the situation near Tc0 .