High Temperature Copper Oxide Superconductors: Properties, Theory and Applications in Society Presented by Thomas Hines in partial fulfillment of Physics.

Slides:



Advertisements
Similar presentations
Trapped ultracold atoms: Bosons Bose-Einstein condensation of a dilute bosonic gas Probe of superfluidity: vortices.
Advertisements

High T c Superconductors & QED 3 theory of the cuprates Tami Pereg-Barnea
c18cof01 Magnetic Properties Iron single crystal photomicrographs
P461 - Semiconductors1 Superconductivity Resistance goes to 0 below a critical temperature T c element T c resistivity (T=300) Ag mOhms/m Cu
Thermomechanical Processing of High T c Superconducting Wire Super BSCCO Family C. Bjelkengren B. Cooper Y. King S. Maltas.
High Temperature Superconductivity: The Secret Life of Electrons in Cuprate Oxides.
Superconductivity David Kelley ECPE
Semiconductors n D*n If T>0
Free electrons – or simple metals Isolated atom – or good insulator From Isolation to Interaction Rock Salt Sodium Electron (“Bloch”) waves Localised electrons.
The Three Hallmarks of Superconductivity
26-29 Nov Superconducting magnetic levitated bearings for rotary machines Superconducting magnetic levitated bearings for rotary machines 5 th.
Superconductor Ceramics
Advanced Higher Chemistry
Superconductivity Characterized by- critical temperature T c - sudden loss of electrical resistance - expulsion of magnetic fields (Meissner Effect) Type.
Vortex Dynamics in Type II Superconductors Yuri V. Artemov Yuri V. Artemov Ph.D. Student in Physics Brian B. Schwartz Mentor: Brian B. Schwartz Professor.
A1- What is the pairing mechanism leading to / responsible for high T c superconductivity ? A2- What is the pairing mechanism in the cuprates ? What would.
Subir Sachdev Yale University Phases and phase transitions of quantum materials Talk online: or Search for Sachdev on.
Magnetic Properties of Materials
Superconductors: Basic Concepts Daniel Shantsev AMCS group Department of Physics University of Oslo History Superconducting materials Properties Understanding.
Metals: Free Electron Model Physics 355. Free Electron Model Schematic model of metallic crystal, such as Na, Li, K, etc.
Superconducting Qubits Kyle Garton Physics C191 Fall 2009.
Investigations in Superconductivity Lulu Liu Partner: Chris Chronopoulos 8.14 Experiment 4 May 12, 2008.
High Temperature Superconductivity Allen Moussa
Superconductors and their applications
By: Shruti Sheladia, Garrett M Leavitt, Stephanie Schroeder, Christopher Dunn, Kathleen Brackney Levitation of a magnet above a high temperature superconductor.
Resistance R - _____________________________________ ____________________________________________________ _____________________________________________________.
Who was the first person to observe superconductivity? 1.Leon Cooper 2.Walther Meissner 3.Sir James Dewar 4.Heike Kamerlingh- Onnes.
How does Superconductivity Work? Thomas A. Maier.
MgB2 Since 1973 the limiting transition temperature in conventional alloys and metals was 23K, first set by Nb3Ge, and then equaled by an Y-Pd-B-C compound.
Superconductors Jason Weimer Honors physics Mr. Pagani Period 3 Project A.
Cultural Project 1- Superconductors Molly Risko Xinyu Zhu Evonne Britton Shu Chen.
Dung-Hai Lee U.C. Berkeley Quantum state that never condenses Condense = develop some kind of order.
Superconductors J Pemberton Dutch Physicist Fredrick Onnes was measuring the resistivity of Mercury and found it went to zero at 4K.
Pressure effect on electrical conductivity of Mott insulator “Ba 2 IrO 4 ” Shimizu lab. ORII Daisuke 1.
Michael Browne 11/26/2007.
Studies of the Cryogenic Part with Load Lock System T. Eisel, F. Haug CERN TE-CRG-CI October 19 th, 2011, Page 1 Superconductivity years Heike Kamerlingh.
Superconductivity and Superfluidity PHYS3430 Professor Bob Cywinski “Superconductivity is perhaps the most remarkable physical property in the Universe”
Non-Fermi Liquid Behavior in Weak Itinerant Ferromagnet MnSi Nirmal Ghimire April 20, 2010 In Class Presentation Solid State Physics II Instructor: Elbio.
c18cof01 Magnetic Properties Iron single crystal photomicrographs
Superconductivity. Work on Worksheets. Superconductivity Lecture
Superconducting Cobaltites Nick Vence. Definition A material which looses its electrical resistivity below a certain temperature (Tc)is said to be superconducting.
SUPERCONDUCTORS mobile electrons in conducting material move through lattice of atoms or ions that vibrate (thermal motion) when conductor is cooled down.
Why Make Holes in Superconductors? Saturday Morning Physics December 6, 2003 Dr. Sa-Lin Cheng Bernstein.
Resistance R - _____________________________________ ____________________________________________________ _____________________________________________________.
Chapter 7 in the textbook Introduction and Survey Current density:
Page 1 Jean Delayen Center for Accelerator Science Old Dominion University and Thomas Jefferson National Accelerator Facility SURFACE IMPEDANCE COCKCROFT.
HIGH TEMPERATURE SUPERCONDUCTORS. INTRODUCTION Superconducitivity Beginning of HTS.
Superconductivity Basics
Superconductivity and Superfluidity The Microscopic Origins of Superconductivity The story so far -what do we know about superconductors?: (i) Superconductors.
Superconductivity Eton College Physics WJEC AS Level.
HIGH TEMPERATURE SUPERCONDUCTOR Prepared By Dutt Thakar.
WHAT IS SUPERCONDUCTIVITY?? For some materials, the resistivity vanishes at some low temperature: they become superconducting. Superconductivity is the.
Superconductor Ceramics
Dipole magnets A dipole magnet gives a constant B-field.
Toward a Holographic Model of d-wave Superconductors
Super Conductivity/ Quantum Locking
BCS THEORY BCS theory is the first microscopic theory of superconductivity since its discovery in It explains, The interaction of phonons and electrons.
Nathan Finney Michael Gammon Newell Jensen
Electrons-electrons interaction
Topological Phase transitions and Topological phases of matter
Spontaneous Symmetry Breaking and Analogies to the Higgs-Mechanism
Electrical Properties of Materials
Experimental Evidences on Spin-Charge Separation
General Outcome #1: Investigate technologies that transfer and control electricity.
…And Men With Funny Hats. …Superconductors… …Semiconductors…
Superconductivity Res. T
Magnetic Properties and Superconductivity
A. J. Leggett University of Illinois at Urbana-Champaign
Ginzburg-Landau theory
Presentation transcript:

High Temperature Copper Oxide Superconductors: Properties, Theory and Applications in Society Presented by Thomas Hines in partial fulfillment of Physics 335

Introduction Superconductors have a critical temperature, magnetic field and current, all of which must not be exceeded for superconductive behavior to be observed Superconductors are characterized by the complete absence of electrical resistivity below a given temperature.

Type I Superconductors Usual composition is Metals and Metalloids Characterized by low critical temperatures Operate on BCS Theory, named after Bardeen, Cooper Schieffer

BCS Theory Electrons couple to form Cooper pairs with energy close to the Fermi level, the higest energy an electron can have at 0 degrees Kelvin. These Cooper pairs act like bosons and propagate through the crystal by inducing resonance.

Type II Superconductors Characterized by much higher critical temperatures than type I, often exceeding 77 K, the boiling point of nitrogen. Many type II superconductors are metal oxides known as perovskites, containing two metal atoms for every three oxygen atoms Electrons form pairs, but the pairing mechanism is different than that described by BCS theory

Type II Superconductors continued Undergo a mixed state of superconductivity between upper and lower critical magnetic fields

Type II properties Meisner Effect Exhibition of diamagnetic properties, defined as the expulsion of magnetic flux from penetrating the material Most superconductors are not completely diamagnetic

Type II Properties Flux Pinning A phenomenon in which magnetic flux becomes trapped or pinned inside the superconducting material Requires defects to be present in the material Necessary to prevent the emergence of pseudo resistance and to keep critical current and critical magnetic field from dropping.

Type II Properties Anisotropy Critical magnetic field dependence on which direction external magnetic field is applied relative to crystallographic orientation Results from the CuO layer (conducting layer) in the crystal spanning only two dimensions Generally speaking, the more anisotropic a superconductor is, the higher critical temperature it will have

Type II Properties Vortices Swirls of electric current induced by the application of an external magnetic field Superconductive behavior is microscopically suppressed in vortices resulting in a mixed state behavior Complete superconductive behavior is lost when vortices overlap

Type II Properties

Theory – What is Generally Agreed Upon Electron vacancies within the CuO layer of the crystal are thought to be charge carriers (although in Ln 2- X Ce X CuO 4-Y, experiments show electrons are the charge carriers). During the Mott transition, holes from blocking layers dope the CuO layer to alter its conductivity.

Theory – Blackstead Dow Chain layer (plane containing CuO is compressed by surrounding cuprate planes into the superconducting state. Accounts for apparent unbalance of charge in ceramic superconducting compounds Supported by the experimental observation that the chain layer is sensitive to magnetism, and the cuprate plane is not.

Theory - Todura Takag Uchida Theorizes that an electron factionalizes into a neutral spin half fermion called a “spinon” and a spinless “holon” or “chargon” with charge e. Inspired by the observation that fermions do not carry heat in high temperature superconductors and attempts to fit this with Wiedmann- Franz Law. Wiedmann- Franz Law predicts that both heat and charge a transported via a single “quasiparticle”.

Theory – Magnetic Resonance When bombarded with neutrons, Cooper spins responded as a group by entering a magnetic resonance mode Shows that spins are strongly interacting and could hold cooper pairs together.

Applications MAGLEV trains Magnetic Resonance Imaging SQUID – Superconducting Quantum Interface Device Particle accelerators Electric generators (up to 99% efficient) Distributed Superconducting Magnetic Energy Storage System (D-SMES) Microchips – up to 1000 teraflops E Bombs – create a strong EM pulse to disable electronics

Applications Superconducting Cables Multifilament wire or tape composed of Cu or Ag matrix embedded with superconducting filaments Matrix impedes penetration of magnetic flux from one superconducting filament to another

Applications Projected worth of superconductor market at current growth rate

Questions?