L.Ya. Vinnikov   L.A, Emelchenko ISSP RAS, Chernogolovka, RUSSIA

Slides:



Advertisements
Similar presentations
Critical Fields and Critical Currents in MgB 2 David Caplin and Judith Driscoll Imperial College, London Work supported by EPSRC Commercial Uses of Magnesium.
Advertisements

Superconductors. Gor’kov and Eliashberg found the time- dependent G-L equations using microscopic theory: These equations are solved numerically Model.
Title Vortex matter in presence of disorder Eli Zeldov Weizmann Institute of Science Rehovot, Israel.
Two Major Open Physics Issues in RF Superconductivity H. Padamsee & J
INSTITUT MAX VON LAUE - PAUL LANGEVIN Penetration Depth Anisotropy in MgB 2 Powder Measured by Small-Angle Neutron Scattering by Bob Cubitt & Charles Dewhurst.
高温超導的量子磁通状態和相変 胡 暁 計算材料科学研究中心 物質・材料研究機構、日本筑波    hc/2e |||| B JsJs  Vortex states and phase transitions in high-Tc superconductivity Xiao Hu National.
High T c Superconductors in Magnetic Fields T. P. Devereaux.
Probing Superconductors using Point Contact Andreev Reflection Pratap Raychaudhuri Tata Institute of Fundamental Research Mumbai Collaborators: Gap anisotropy.
High T c Superconductors & QED 3 theory of the cuprates Tami Pereg-Barnea
Kitaoka lab Itohara Keita
 Single crystals of YBCO: P. Lejay (Grenoble), D. Colson, A. Forget (SPEC)  Electron irradiation Laboratoire des Solides Irradiés (Ecole Polytechnique)
1 In a vortex system a force applied on a vortex by all the others can be written within London appr. as a sum: IV. FLUX LINE LATTICE The total energy.
1 Most of the type II superconductors are anisotropic. In extreme cases of layered high Tc materials like BSCCO the anisotropy is so large that the material.
Multiple phase transformations in weakly pinned vortex matter S. Ramakrishnan and A. K. Grover S. Ramakrishnan and A. K. Grover Department of Condensed.
Size effect in the vortex-matter phase transition in Bi 2 Sr 2 CaCuO 8+  ? B. Kalisky, A. Shaulov and Y. Yeshurun Bar-Ilan University Israel T. Tamegai.
Bardeen-Stephen flux flow law disobeyed in Bi 2 Sr 2 CaCu 2 O 8+δ G. Kriza, 1,2 A. Pallinger 1, B. Sas 1, I. Pethes 1, K. Vad 3, F. I. B.Williams 1,4 1.
Small-Angle Neutron Scattering & The Superconducting Vortex Lattice
Zero Field Superconducting Transition with Columnar Defects A. Vestergren, Mats WallinS. TeitelHans Weber KTH, StockholmUniver. RochesterLuleå Univer.
Vortex Pinning and Sliding in Superconductors Charles Simon, laboratoire CRISMAT, CNRS.
cond-mat/ , cond-mat/ , and to appear
Phase Diagram of a Point Disordered Model Type-II Superconductor Peter Olsson Stephen Teitel Umeå University University of Rochester IVW-10 Mumbai, India.
1 L.D. Landau ( 1937 ) A second order phase transition is generally well described phenomenologically if one identifies: a). The order parameter field.
Classifying two-dimensional superfluids: why there is more to cuprate superconductivity than the condensation of charge -2e Cooper pairs cond-mat/ ,
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.
Antiferomagnetism and triplet superconductivity in Bechgaard salts
Flux pinning in general Adrian Crisan School of Metallurgy and Materials, University of Birmingham, UK and National Institute of Materials Physics, Bucharest,
Condensed Matter Physics Big Facility Physics26th Jan 2004 Sub Heading “Big Facility” Physics in Grenoble ESRF: X-rays ILL: neutrons.
Ying Chen Los Alamos National Laboratory Collaborators: Wei Bao Los Alamos National Laboratory Emilio Lorenzo CNRS, Grenoble, France Yiming Qiu National.
Microscopic nematicity in iron superconductors Belén Valenzuela Instituto de Ciencias Materiales de Madrid (ICMM-CSIC) In collaboration with: Laura Fanfarillo.
Title Vortex nanoliquid in high-temperature superconductors.
A image of the flux line lattice in the magnetic superconductor TmNi2B2C The hexagonal arrangement of magnetic flux lines in pure Nb imaged using neutrons.
1 Superconductivity  pure metal metal with impurities 0.1 K Electrical resistance  is a material constant (isotopic shift of the critical temperature)
I. Grigorieva, L. Vinnikov, A. Geim (Manchester) V. Oboznov, S. Dubonos (Chernogolovka)
Studies on supercooled metastable states of vortex matter P Chaddah Cryogenics & Superconductivity Section, Centre for Advanced Technology, Indore
Don McKenzie Paul University of Warwick Don McKenzie Paul University of Warwick The Vortex Lattice in Superconductors as seen by neutron diffraction An.
Colossal Magnetoresistance of Me x Mn 1-x S (Me = Fe, Cr) Sulfides G. A. Petrakovskii et al., JETP Lett. 72, 70 (2000) Y. Morimoto et al., Nature 380,
Pressure effect on electrical conductivity of Mott insulator “Ba 2 IrO 4 ” Shimizu lab. ORII Daisuke 1.
Structure in the mixed phase
Superconducting vortex avalanches D. Shantsev Åge A. F. Olsen, D. Denisov, V. Yurchenko, Y. M. Galperin, T. H. Johansen AMCS (COMPLEX) group Department.
Coexistence and Competition of Superconductivity and Magnetism in Ho 1-x Dy x Ni 2 B 2 C Hyeon-Jin Doh, Jae-Hyuk Choi, Heon-Jung Kim, Eun Mi Choi, H. B.
Michael Browne 11/26/2007.
Phase diagram of solid oxygen at low temperature and high pressure
Magneto-optical imaging of Superconductors Satyajit S.Banerjee Dept of Physics, Indian Institute of Technology, Kanpur, India.
Dendritic Thermo-magnetic Instability in Superconductors Daniel V. Shantsev AMCS group, Department of Physics, UiO Collaboration: D. V. Denisov, A.A.F.Olsen,
National Science Foundation X-ray vision of nano-materials Eric E Fullerton, University of California-San Diego, DMR Researcher at University of.
P. M. Grant Superconductivity 101 Superconductivity Workshop Charlotte, 24 May 1999 Superconductivity 101 A Primer for Engineers Paul M. Grant
Introduction to Molecular Magnets Jason T. Haraldsen Advanced Solid State II 4/17/2007.
Vortex avalanches in superconductors: Size distribution and Mechanism Daniel Shantsev Tom Johansen andYuri Galperin AMCS group Department of Physics, University.
Peak effect in Superconductors - Experimental aspects G. Ravikumar Technical Physics & Prototype Engineering Division, Bhabha Atomic Research Centre, Mumbai.
Critical state controlled by microscopic flux jumps in superconductors
I NTERLAYER E XCHANGE C OUPLING, P AIR B REAKING & 2D V ORTEX D YNAMICS IN F ERROMAGNET - S UPERCONDUCTOR H ETEROSTRUCTURES R. C. B UDHANI Indian Institute.
Emergent Nematic State in Iron-based Superconductors
Magnetic Frustration at Triple-Axis  Magnetism, Neutron Scattering, Geometrical Frustration  ZnCr 2 O 4 : The Most Frustrated Magnet How are the fluctuating.
Vortex Lattice Anisotropy in Magnesium Diboride Morten Ring Eskildsen Department of Physics University of Notre Dame.
Antiferromagnetic Resonances and Lattice & Electronic Anisotropy Effects in Detwinned La 2-x Sr x CuO 4 Crystals Crystals: Yoichi Ando & Seiki Komyia Adrian.
SUMMARY Magneto-optical studies of a c-oriented epitaxial MgB 2 film show that below 10K the global penetration of vortices is dominated by complex dendritic.
Why Make Holes in Superconductors? Saturday Morning Physics December 6, 2003 Dr. Sa-Lin Cheng Bernstein.
Anomalous Local Transport in MicrofabricatedSr 2 RuO 4 -Ru Eutectic Junction Univ. AISTHiroshi Kambara Satoshi Kashiwaya Tokyo.
Pinning Effect on Niobium Superconducting Thin Films with Artificial Pinning Centers. Lance Horng, J. C. Wu, B. H. Lin, P. C. Kang, J. C. Wang, and C.
1 Vortex configuration of bosons in an optical lattice Boulder Summer School, July, 2004 Congjun Wu Kavli Institute for Theoretical Physics, UCSB Ref:
Transport Measurements in Superconductivity and DC Magnetization
Phase Diagram of Ruthenate: Ca2-xSrxRuO4 (CSRO) (0. 0<x<2
Super Conductivity/ Quantum Locking
M. RIESTER , H. BÖHM and V. PETRICEK‡ contact:
Scientific Achievement
Scientific Achievement
Special Topics in Electrodynamics:
Quasi One-Dimensional Vortex Flow Driven Through Mesoscopic Channels
Special Topics in Electrodynamics:
Ginzburg-Landau theory
Presentation transcript:

Visualization Abrikosov’s Vortices by Decoration Method in Novel Superconductors L.Ya. Vinnikov   L.A, Emelchenko ISSP RAS, Chernogolovka, RUSSIA F.L. Barkov J.Karpinskii ETH-Zurich, SWITZERLAND S.M.Kazakov J. Jun J.Anderegg AMESLAB,ISU, AMES, USA S.L.Budko P.C.Canfield V.Kogan

History(outline) Add pictures –vortex pinning for YBCO123 by twin boundaries

Anisotropy FLL in YBCO (ab) plane YBCO 123 YBCO 124

Vortex pinning by twin boundaries in YBCO123

Flux Line Lattice destruction by columnar defects in BSCCO

Observation flux Line Lattice in the Organic Superconductors

Vortices in MgB2

The VL in LuNi2B2C for B=1840 Gs Add data V3Si ? The right insert is the Fourier transform, the left one autocorrelation pattern

Anisotropy in the long-range order LuNi2B2C V3Si PRB (2000) Anisotropy in the long-range order

RHOMBIC -TO–SQUARE VORTEX LATTICE TRANSITION PRB (2000) LuNi2B2C V3Si

N. Saha, R.Surdeanu, M.Marchevsky et al PRB (2000)

Vortex Structure in ErNi2B2C H=8 Oe, Td=5.5K

Vortex Structure in HoNi2B2C H= 17 Oe, Td= 4.3K

Magnetoelastic tetragonal-to-orthorhombic distortion for RNi2B2C

Magnetic structure for RNi2B2C

Superconducting and antiferromagnetic transition for RNi2B2C

Magnetic Flux Structure in TbNi2B2C The direct evidence for magnetic nature of the pinning by twin boundaries in RNi2B2C R=Er (at least partial)

SUMMARY The Bitter decoration provides a distinctive high-resolution technique for observation of anisotropy FLL, vortex pinning as well as antiferromagnetic domain in magnetic superconductors.   We have observed magnetic (vortex) structure for wide range magnetic fields and temperatures for superconducting and normal states for family RNi2B2C single crystals . We find the crystalographic ordered vortex structures in HoNi2B2C and ErNi2B2C result from pinning by magnetic twin boundaries in antiferromagnetic state. The domain magnetic structure have revealed in AF state in TbNi2B2C for the first time by Bitter decoration technique. Taking to account the symmetry of magnetoelastic distortions at AF transition in RNi2B2C we can predict that for DyNi2B2C at temperatures less than TN should be observed structures similar observed here for HoNi2B2C