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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Superconductivity 101 A Primer for Engineers Paul M. Grant pgrant@epri.com www.epri.com/staff_papers/sst
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Fathers of Electricity Discoverers
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Fathers of Electricity Practitioners
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Fathers of Cryogenics DewarKammerlingh-Onnes CH 4 112 K O 90 N 2 77 Ne 27 H 2 20 He 4.2
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 ( ( ( Models of Electrical Conductivity The First Idea: R T Just Goes to Zero! ((( ( ( ( ( ( ( e-e- e-e-
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 The Most Popular: R T Freezes Out! e-e- Models of Electrical Conductivity
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Models of Electrical Conductivity Reality: R T Limited by Impurities! e-e-
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Thus the mercury at 4.2 K has entered a new state, which, owing to its particular electrical properties, can be called the state of superconductivity H. Kamerlingh-Onnes (1911) 1911 A Big Surprise!
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Magnetic Properties 0 -1/4 T H off H on 0 -1/4 T H on Expected (Lenz’ Law) Weird ! (Meissner Effect)
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 They all tried… and failed!
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 They came close... Fritz London Lev Landau Irwin Froehlich “The B-field does penetrate.” E ~ 2 dJ/dt, B ~ 2 J “Since SC is a second-order phase transition, there must be an order parameter involved.” “T C depends on the mass of the atoms (isotope effect), so the SC must be tied to lattice vibrations (phonons).”
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 They Got It Right! B ----- C ----- S Bardeen: “It’s a macroscopic quantum state” Cooper: “It’s got twice the charge you’d expect” Schrieffer: “ ’s a statistical wavefunction” There has to be a regime where the lattice vibrations act to bind electrons together rather than scatter them with loss as given by Ohm’s Law.
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Physics of Superconductivity ++ ++ e-e- e-e- Electrons Pair Off! BCS Equation
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 “Cooper’s Problem”
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Important Numbers in Superconductivity Transition Temperature, T C Way below 300 K Critical Current Density, J C 10 -2 - 10 6 A/cm 2 Critical Magnetic Field, H C 10 -4 - 10 T London Penetration Depth, 10 - >1000 Å Pippard Coherence Length, 10 - >1000 Å G-L Parameter, = / 0.01 - 100 NB! All these numbers depend on each other. E.g., H C ~
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 T C vs. Year: 1911 - 1980 Year 0 5 10 15 20 25 190019101920193019401950196019701980 Temperature (K) Hg Pb NbN V 3 Si Nb 3 Sn Nb 3 Ge Cubic Metals
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 MRI & “Big Physics” Magnetic Resonance Imaging Philips Tevatron Fermi National Laboratory
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 1986 Another Big Surprise! Bednorz and Mueller IBM Zuerich, 1986 Onset T C = 40 K !
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 1987 “The Prize!”
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 March 3, 1987 “123” Discovered
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Woodstock of Physics NYC, 1987 Physicists’ Night Out!
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Y-123Bi-2223 HTS Layered Perovskites
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 T C vs. Year: 1911 - 1999 190019201940196019802000 0 50 100 150 200 Temperature, T C (K) Year Low-T C High-T C 164 K
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 HTSC Phase Diagram
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 HTS Theories Phil Anderson “It can’t be just an accident that high temperature superconductivity occurs in a host material whose insulating state is an antiferromagnet, and, which when doped with holes to a level where magnetic behavior disappears, we get superconductivity.” Current Situation: The pair coupling is believed to be magnetically mediated. The normal conducting state is believed not to be a Landau liquid. The superconducting state is domain- like, occurring as electronic “stripes.” However, there is yet no generally accepted model today!
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Boson Flavors
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Ultimate Boson Put-ons!
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 GLAG Lev Gor’kov
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Irreversibility Line Mixed Normal H C2 Magnetic Field TCTC Temperature H C2 1/4 Type II Superconductivity Mixed H C2 Meissner H C1 H C2 Normal
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Abrikosov Vortex Lattice Dipole Force F Lorentz J H Type II Superconductor in the Mixed State
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Hg-1212: Fission-Induced Defects L. Krusin-Elbaum, et al., Nature World record H irr at 77 K in Hg-1212 Hg-1212 Prototype Tapes made at TCSUH Potential for high- field magnet inserts
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Extrinsic Pinning 10 m m DECORATED VORTEX ARRAYS with random heavy ion tracks clean M. Leghissa, et al. Phys. Rev.B48, 1341 (1993)
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Vortex Matter Static Phase Diagram Temperature Magnetic Field Dynamic Phase Diagram TCTC H C2 H C1 F Lorentz Elastic Flow Plastic Flow Liquid Flow Normal Liquid Glass Solid Bose Glass Polymer Glass Melting Line Meissner State SC Fluctuation Regime
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 J C (B,T) for BSCCO
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 BSCCO OPIT/Ag E-J Characteristic E = aJ n n = 15 T = 77 K E = 1 V/cm
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Solenoid Loop Current: t > t 0 L R(I) I(t) bIL dI dt 0 I(t) b(n1) L (tt)I n 00 1n 1 1n
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 “Persistent” Current Decay B = 0.50 T B = 0.25 T 12 Days
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Type II Hysteresis H M
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Hysteretic ac Loss
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 The Future 2028
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 The Future 700 K ! May, 2028
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Electricity: A Life Necessity California, Summer 1996 Quebec, Winter 1997
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 “You can’t always get what you want…”
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P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 “…you get what you need!”
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