logging in or signing up bernsteintwo Arkwright26 Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 188 Category: Entertainment License: All Rights Reserved Like it (0) Dislike it (0) Added: October 16, 2007 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Why Make Holes in Superconductors?: Why Make Holes in Superconductors? Saturday Morning Physics December 6, 2003 Dr. Sa-Lin Cheng BernsteinType I Superconductors: Type I Superconductors Two Conditions: Zero resistivity Meissner effect Superconducting state: T < Tc H < Hc Theoretical Understanding: Theoretical Understanding 1930s – quantum model could not explain superconductivity 1950 – phenomenological theory by Vitaly Ginzburg and Lev Landau Ginzburg-Landau equation Describe superconductivity near Tc 2003 – Ginzburg wins Nobel Prize in physics (Nobel Lectures will be held on December 8)Vitaly L. Ginzburg:: Vitaly L. Ginzburg: The New York Times, October 8, 2003 "They have been nominating me for about 30 years, so in that sense it didn't come out of the blue. But I thought, `Well, they're not giving it to me, I guess that's it.' After all, there are a lot of contenders. So, you know, I had long ago forgotten to think about this."BCS Theory: BCS Theory BCS = John Bardeen, Leon Cooper, and Robert Schrieffer 1957 – explain why superconductivity occurs Cooper pairs = Pairing of electrons 1972 – Nobel Prize in physics http://superconductors.orgCritical Fields in Type II: Critical Fields in Type II Lower critical field Upper critical field vortices Incomplete Meissner Effect Mixed State in Type II : Mixed State in Type II Hc1< H < Hc2 Also called “vortex state” Magnetic field can penetrate but not completely Flux lines D. J. Bishop et al., © Scientific American, 48 (Feb. 1993) Abrikosov Vortex Lattice: Abrikosov Vortex Lattice 1953 – Abrikosov Vortex Lattice Based on Ginzburg – Landau equation Flux lines repel each other Triangular vortex lattice 2003 – Nobel Prize in physics A. A. Abrikosov © AT&T, 1995Nobel Prize Winning: Nobel Prize WinningAbrikosov Lattice Images: Abrikosov Lattice Images First image of Vortex lattice, 1967 Bitter Decoration Pb-4at%In rod, 1.1K, 195G U. Essmann and H. Trauble © Physics Letters 24A, 526 (1967) Vortices in MgB2, 2002 Scanning Tunnel Spectroscopy MgB2 crystal, 2K, 2000G M. R. Eskildsen et al. © Phys. Rev. Lett. 89, 187003 (2002) What is a vortex?: What is a vortex? Photo courtesy of the National Severe Storms Laboratory Vortex (flux line) in superconductor: Vortex (flux line) in superconductor Has a core, circled by supercurrents Inside the core: normal electrons Outside the core: superconducting electrons (Cooper pairs) Examples of Type II: Examples of Type II Mostly compounds Record holder: Tc =138 K High Hc2: Hc2 > 1000 000 G (YBCO) See the Light . . .: See the Light . . . More useful higher Tc higher Hc2 Easily cooled: He (4.22 K): $5/liter N (77.36 K): 10¢/liter whole milk: 66¢/liter Columbia Pictures The Fifth Element The “but”. . .: The “but”. . . Dilemma of Type II superconductors Solutions?Magnetic Force on Current: Magnetic Force on Current Thumb = current Fingers = magnetic field Palm = magnetic force Lorentz force © John Wiley & Sons, Inc.Superconducting Wires: Superconducting Wires Top View Magnetic field: out of page D. J. Bishop et al., © Scientific American, 48 (Feb. 1993) Resistance in Superconductors: Resistance in Superconductors Lorentz force pushes vortices (Flux motion) Dissipation of energy Resistance Increase of temperature Quench!!! Critical Surface Phase Diagram: Critical Surface Phase Diagram Superconducting state: T < Tc H < Hc J < Jc Dilemma: Dilemma For practical applications, high Tc high Hc high Jc Dilemma: highest Jc is at Tc=0 and Hc=0 Solution: Solution Prevent flux from moving Tarp (or pin) flux Flux Pinning: Flux Pinning Defects in crystalline structure Impurities Grain boundaries Artificial pinning centers: Holes (antidots) Magnetic dots Arrays of dots Single defect in a YBa2Cu3O7 film (magneto-optical imaging) http://www.fys.uio.no/super/mo/Energy Surface: Energy Surface Potential energy drops discontinuously when the vortex enters the defect zoneExperiment Evidence: Experiment Evidence Rectangular array of antidots http://www.fys.kuleuven.ac.be/vsm/nsm/research/lieve2.htmlInterstitial Vortices: Reside in the area between pinning sites Trapped by other vortices (due to mutual repulsion) More mobile Energy Dissipation!! Interstitial Vortices http://www.physics.colostate.edu/groups/fieldgroup/Holes.htmlSolution: Solution Large defects Solution2: Solution2 Magnetic pinning centersSummary: Summary Type II superconductor: Incomplete Meissner effect in vortex state (Hc1 < H < Hc2) Superconducting state: T < Tc H < Hc2 J < Jc Flux consists of whirlpools supercurrent called vortex Abrikosov vortex lattice = triangular array Interstitial vortices are mobile energy lost Effective pinning centers: Larger size Magnetic dots Summary You do not have the permission to view this presentation. In order to view it, please contact the author of the presentation.
bernsteintwo Arkwright26 Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 188 Category: Entertainment License: All Rights Reserved Like it (0) Dislike it (0) Added: October 16, 2007 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Why Make Holes in Superconductors?: Why Make Holes in Superconductors? Saturday Morning Physics December 6, 2003 Dr. Sa-Lin Cheng BernsteinType I Superconductors: Type I Superconductors Two Conditions: Zero resistivity Meissner effect Superconducting state: T < Tc H < Hc Theoretical Understanding: Theoretical Understanding 1930s – quantum model could not explain superconductivity 1950 – phenomenological theory by Vitaly Ginzburg and Lev Landau Ginzburg-Landau equation Describe superconductivity near Tc 2003 – Ginzburg wins Nobel Prize in physics (Nobel Lectures will be held on December 8)Vitaly L. Ginzburg:: Vitaly L. Ginzburg: The New York Times, October 8, 2003 "They have been nominating me for about 30 years, so in that sense it didn't come out of the blue. But I thought, `Well, they're not giving it to me, I guess that's it.' After all, there are a lot of contenders. So, you know, I had long ago forgotten to think about this."BCS Theory: BCS Theory BCS = John Bardeen, Leon Cooper, and Robert Schrieffer 1957 – explain why superconductivity occurs Cooper pairs = Pairing of electrons 1972 – Nobel Prize in physics http://superconductors.orgCritical Fields in Type II: Critical Fields in Type II Lower critical field Upper critical field vortices Incomplete Meissner Effect Mixed State in Type II : Mixed State in Type II Hc1< H < Hc2 Also called “vortex state” Magnetic field can penetrate but not completely Flux lines D. J. Bishop et al., © Scientific American, 48 (Feb. 1993) Abrikosov Vortex Lattice: Abrikosov Vortex Lattice 1953 – Abrikosov Vortex Lattice Based on Ginzburg – Landau equation Flux lines repel each other Triangular vortex lattice 2003 – Nobel Prize in physics A. A. Abrikosov © AT&T, 1995Nobel Prize Winning: Nobel Prize WinningAbrikosov Lattice Images: Abrikosov Lattice Images First image of Vortex lattice, 1967 Bitter Decoration Pb-4at%In rod, 1.1K, 195G U. Essmann and H. Trauble © Physics Letters 24A, 526 (1967) Vortices in MgB2, 2002 Scanning Tunnel Spectroscopy MgB2 crystal, 2K, 2000G M. R. Eskildsen et al. © Phys. Rev. Lett. 89, 187003 (2002) What is a vortex?: What is a vortex? Photo courtesy of the National Severe Storms Laboratory Vortex (flux line) in superconductor: Vortex (flux line) in superconductor Has a core, circled by supercurrents Inside the core: normal electrons Outside the core: superconducting electrons (Cooper pairs) Examples of Type II: Examples of Type II Mostly compounds Record holder: Tc =138 K High Hc2: Hc2 > 1000 000 G (YBCO) See the Light . . .: See the Light . . . More useful higher Tc higher Hc2 Easily cooled: He (4.22 K): $5/liter N (77.36 K): 10¢/liter whole milk: 66¢/liter Columbia Pictures The Fifth Element The “but”. . .: The “but”. . . Dilemma of Type II superconductors Solutions?Magnetic Force on Current: Magnetic Force on Current Thumb = current Fingers = magnetic field Palm = magnetic force Lorentz force © John Wiley & Sons, Inc.Superconducting Wires: Superconducting Wires Top View Magnetic field: out of page D. J. Bishop et al., © Scientific American, 48 (Feb. 1993) Resistance in Superconductors: Resistance in Superconductors Lorentz force pushes vortices (Flux motion) Dissipation of energy Resistance Increase of temperature Quench!!! Critical Surface Phase Diagram: Critical Surface Phase Diagram Superconducting state: T < Tc H < Hc J < Jc Dilemma: Dilemma For practical applications, high Tc high Hc high Jc Dilemma: highest Jc is at Tc=0 and Hc=0 Solution: Solution Prevent flux from moving Tarp (or pin) flux Flux Pinning: Flux Pinning Defects in crystalline structure Impurities Grain boundaries Artificial pinning centers: Holes (antidots) Magnetic dots Arrays of dots Single defect in a YBa2Cu3O7 film (magneto-optical imaging) http://www.fys.uio.no/super/mo/Energy Surface: Energy Surface Potential energy drops discontinuously when the vortex enters the defect zoneExperiment Evidence: Experiment Evidence Rectangular array of antidots http://www.fys.kuleuven.ac.be/vsm/nsm/research/lieve2.htmlInterstitial Vortices: Reside in the area between pinning sites Trapped by other vortices (due to mutual repulsion) More mobile Energy Dissipation!! Interstitial Vortices http://www.physics.colostate.edu/groups/fieldgroup/Holes.htmlSolution: Solution Large defects Solution2: Solution2 Magnetic pinning centersSummary: Summary Type II superconductor: Incomplete Meissner effect in vortex state (Hc1 < H < Hc2) Superconducting state: T < Tc H < Hc2 J < Jc Flux consists of whirlpools supercurrent called vortex Abrikosov vortex lattice = triangular array Interstitial vortices are mobile energy lost Effective pinning centers: Larger size Magnetic dots Summary