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Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang. Lecture 5 Superconductivity Flux Quantization & SQUID. Kammerlingh Onnes 1853-1926 On the Sudden Rate at Which the Resistance of Mercury Disappears Communications of the Leiden Laboratory, 1911.
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Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang Lecture 5 Superconductivity Flux Quantization & SQUID
Kammerlingh Onnes 1853-1926 On the Sudden Rate at Which the Resistance of Mercury Disappears Communications of the Leiden Laboratory, 1911
Meissner Effect 1933 Robert Ochsenfeld Walther Meissner 1882 - 1974
Drude’s Theory of Conductivity Perfect conductor Limit
London’s Equations Superconductor Is better than perfect conductor London’s Equation London’s Equation
London Equations Fritz London
John Bardeen Leon Cooper John R. Schrieffer BCS Theory of Superconductivity Phys.Rev.108, 1175 (1957)
Superconductor Charge Density In Absence of Magnetic Field Cooper Pair has zero momentum
In absence of Magnetic Field momentum In presence of Magnetic Field momentum
In the Presence of Magnetic Field Cooper Pair with zero momentum
charge density is constant phase depends on vector potential Superconducting Current Superconducting current
Deep inside fluxoid
Fluxoid Quantization B.Deaver & W. Fairbank Phys Rev Lett 7, 43 (1961)
Brian D. Josephson 1940 -
Vo II I
Vo II I
D.C. Josephson effect Anderson & Rowell experiment, 1963 For V ≠ 0 , JDC = 0 For V = 0 , JDC = Jo sin δo P.W. Anderson
SQUID a Ca P Q Cb b Coupled Josephson Junctions in an external magnetic field
SQUID current for general Flux a Ca P Q Cb b
10-12 August, 2005 Nanyang Technological UniversityNational University of SingaporeBiopolis, A*STAR