'Weak localization' presentation slideshows

Quantum transport and its classical limit

Quantum transport and its classical limit. Piet Brouwer Laboratory of Atomic and Solid State Physics Cornell University. Lecture 1 Capri spring school on Transport in Nanostructures, March 25-31, 2007. Quantum Transport.

748 views • 55 slides

Mesoscopic Anisotropic Magnetoconductance Fluctuations in Ferromagnets

486 views • 39 slides

Disorder and chaos in quantum system: Anderson localization and its generalization

Boris Altshuler (Columbia ). Disorder and chaos in quantum system: Anderson localization and its generalization. (6 lectures). Igor Aleiner (Columbia ). Lecture # 2. Stability of insulators and Anderson transition Stability of metals and weak localization. extended. localized.

309 views • 29 slides

Positive HBT/noise cross-correlations in superconducting hybrids: Role of disorder

Positive HBT/noise cross-correlations in superconducting hybrids: Role of disorder. R. Melin, C. Benjamin and T. Martin, Phys. Rev. B 77, 094512 (2008). Talk outline:. Noise: An Introduction Noise and entanglement: Historical perspective NSN junctions: CAR and EC

326 views • 21 slides

Positive HBT/noise cross-correlations in superconducting hybrids: Role of disorder

Positive HBT/noise cross-correlations in superconducting hybrids: Role of disorder. R. Melin, C. Benjamin and T. Martin, Phys. Rev. B 77, 094512 (2008). Talk outline:. Noise: An Introduction Noise and entanglement: Historical perspective NSN junctions: CAR and EC

321 views • 21 slides

398 views • 18 slides

F.Varchon, L. Magaud cond-mat/0702311

EG1. Linear E(k) Graphene Electron doped. EG2. bilayer layer. Band structure calculations. Graphene layers AB stacked on SiC (bulk terminated Si-face) Density functional theory - VASP code. EG0. Non conducting Buffer layer. Similar results on the SiC C-face.

357 views • 18 slides