High t c superconductors in magnetic fields
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High T c Superconductors in Magnetic Fields. T. P. Devereaux. Kamerlingh Onnes, 1913 Nobel Prize for Discovery of Superconductivity in Mercury. Theory of Superconductivity by Bardeen, Cooper, and Schrieffer Earns Nobel Prize in 1972. Most successful many-body theory. Quantum Coherent State.

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High T c Superconductors in Magnetic Fields

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High t c superconductors in magnetic fields

High Tc Superconductors in Magnetic Fields

T. P. Devereaux


Kamerlingh onnes 1913 nobel prize for discovery of superconductivity in mercury

Kamerlingh Onnes, 1913 Nobel Prize for Discovery of Superconductivity in Mercury


Theory of superconductivity by bardeen cooper and schrieffer earns nobel prize in 1972

Theory of Superconductivity by Bardeen, Cooper, and Schrieffer Earns Nobel Prize in 1972

Most successful many-body theory.

Quantum Coherent State

  • “paired” electrons condense into coherent state -> no resistance.

  • perfect diamagnetism – electrons circulate to screen magnetic field (Meissner effect).


High t c superconductors discovered in 1986 nobel prize for bednorz and m ller in 1987

High Tc Superconductors Discovered in 1986, Nobel Prize for Bednorz and Müller in 1987


Critical current on the rise

Critical Current On the Rise


New superconductor developments

New Superconductor Developments

  • Fullerenes: Tc engineered to 117K.

  • Iron becomes a superconductor under pressure.

  • Plastic superconductor: polythiophene.

  • DNA can be made superconducting.

  • MgB2 changes our thinking (again).


Large scale applications

Large ScaleApplications

Top speed: 552 km/hr

US Navy: 5,000 HP*

In-place in Detroit.*

*American Superconductor Corp.


Small scale devices

Small Scale Devices?

  • Transistors (RSFQ peta-flop supercomputer)?

  • Filters?

  • Nano-scale motors and devices?

  • Superconducting DNA?

  • Quantum computers!?

  • OBSTACLES:

  • cooling.

  • architecture.

  • ever-present magnetic fields destroy coherence.


Small devices magnetic fields

Small Devices? Magnetic Fields!

  • H. Safar et al (1993)

Resistance reappears!

<- Resistivity of Pure Copper


Problem vortices

Problem: Vortices!

Electrons swirl in magnetic field – increased kinetic energy kills superconductivity.

SOLUTION: Magnetic field kills superconductivity in isolated places -> VORTICES (swirling “normal” electrons)


Direct vortex imaging using scanning tunneling microscope

Direct Vortex Imaging Using Scanning Tunneling Microscope


Animation increasing magnetic field

Animation: Increasing Magnetic Field

Apply current: Lorentz force causes vortices to move -> Resistance!


Solution defects to pin vortices

Solution: Defects to Pin Vortices

  • Krusin-Elbaum et al (1996).

  • Critical current enhanced by orders of magnitude over “virgin” material.

  • Splayed defects better than straight ones.

  • Optimal splaying angle ~ 5 degrees.


Animation pinning moving vortices

Animation: Pinning Moving Vortices


Problems to overcome

Problems to Overcome

  • High TC

  • Elastic string under tension F:

Du2= kBTy(L-y)/FL~ kBT/F

String is floppier at higher T -> vortex “liquid”

2) Planar Structure

“pancake” vortices in layers weakly coupled

Decreased string tension -> vortex decoupling


Molecular dynamics simulations

Molecular Dynamics Simulations

  • Widely used for a variety of problems:

    - protein folding, weather simulation, cosmology, chaos, avalanches, marine pollution, other non-equilibrium phenomena.

  • Solves equations of motion for each “particle”.

  • Large scale simulations on pcs and supercomputers (parallel).


Molecular dynamics simulations for vortices

Molecular Dynamics Simulations for Vortices

  • Vortices = elastic strings under tension.

  • Vortices strongly interact (repel each other).

  • Temperature treated as Langevin noise.

  • Solve equations of motion for each vortex.

  • Calculate current versus applied Lorentz force, find what type of disorder gives maximum critical current.


Abrikosov lattice melting vortex liquid

Abrikosov Lattice Melting - > Vortex Liquid

At low T, lattice forms with “defects”.

At higher T, lattice “melts”.


Pinning

Pinning

At low T, a few pins can stop whole “lattice”.

At larger T, pieces of “lattice” shear away.


Pinning at low fields

Pinning at low fields

Columns of defects are effective at pinning vortices.

But “channels” of vortex flow proliferate at larger fields.


Depinning vortex avalanche

Depinning <-> vortex avalanche


Splayed defects effective at cutting off channels of vortex flow

Splayed defects effective at cutting off channels of vortex flow

But too much splaying and vortices cannot accommodate to defects.


Resistivity is smaller for splayed defects

Resistivity is smaller for splayed defects


Optimal angle for splaying

Optimal angle for splaying


Acknowledgement future work

Acknowledgement & Future Work

  • All simulations performed by Dr. C. M. Palmer.

  • Complex vortex dynamics.

  • Future work to investigate

    • Melting phenomena.

    • Oscillatory motion of driven vortices.

    • Onset of avalanches.

    • Behavior as a qubit (quantum computing).

    • Behavior of other dual systems (polymers, DNA,…).


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