第27回応用物理学科セミナー 日時: 10月25日(火) 16:00 – 17:30 場所:葛飾キャンパス研究棟8F第1セミナー室

Slides:



Advertisements
Similar presentations
Department of Physics University of Toronto Low Temperature Thermal Transport Across the Cuprate Phase Diagram Mike Sutherland Louis Taillefer Rob Hill.
Advertisements

Iron pnictides: correlated multiorbital systems Belén Valenzuela Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC) ATOMS 2014, Bariloche Maria José.
High T c Superconductors in Magnetic Fields T. P. Devereaux.
High T c Superconductors & QED 3 theory of the cuprates Tami Pereg-Barnea
Superconductivity Michael Spreitzer. Overview „Superconductivity“ ? Who discovered it ? Meissner & Ochsenknecht effect? BCS – Theory Different types of.
High Temperature Superconductivity: D. Orgad Racah Institute, Hebrew University, Jerusalem Stripes: What are they and why do they occur Basic facts concerning.
Concepts in High Temperature Superconductivity
Oda Migaku STM/STS studies on the inhomogeneous PG, electronic charge order and effective SC gap of high-T c cuprate Bi 2 Sr 2 CaCu 2 O 8+  NDSN2009 Nagoya.
Modeling strongly correlated electron systems using cold atoms Eugene Demler Physics Department Harvard University.
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
High Temperature Copper Oxide Superconductors: Properties, Theory and Applications in Society Presented by Thomas Hines in partial fulfillment of Physics.
Superconductivity Characterized by- critical temperature T c - sudden loss of electrical resistance - expulsion of magnetic fields (Meissner Effect) Type.
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.
Superconducting Qubits Kyle Garton Physics C191 Fall 2009.
Two Particle Response in Cluster Dynamical Mean Field Theory Rosemary F. Wyse, Aspen Center for Physics, PHY/DMR Dynamical Mean Field Theory is.
1 Superconductivity  pure metal metal with impurities 0.1 K Electrical resistance  is a material constant (isotopic shift of the critical temperature)
B. Valenzuela Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC)
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.
SQUIDs (Superconducting QUantum Interference Devices)
Quantum criticality –The physics of quantum critical phase transitions connects to some of the most challenging and technologically relevant problems in.
Michael Browne 11/26/2007.
Unconventional superconductivity Author: Jure Kokalj Mentor: prof. dr. Peter Prelovšek.
Nonlocal quantum coherence between normal probes placed on a superconductor is predicted to occur through two microscopic processes. In crossed Andreev.
Drude weight and optical conductivity of doped graphene Giovanni Vignale, University of Missouri-Columbia, DMR The frequency of long wavelength.
J.P. Eisenstein, Caltech, DMR When two layers of electrons are brought close together in the presence of an intense magnetic field a new state.
Competing Orders, Quantum Criticality, Pseudogap & Magnetic Field-Induced Quantum Fluctuations in Cuprate Superconductors Nai-Chang Yeh, California Institute.
New Ruthenium Oxides: Compounds Poised between Magnetic and Non-magnetic Ground States R. J. Cava, Princeton University, DMR Figuring out the ways.
Development of density functional theory for unconventional superconductors Ryotaro Arita Univ. Tokyo/JST-PRESTO.
Raman Scattering As a Probe of Unconventional Electron Dynamics in the Cuprates Raman Scattering As a Probe of Unconventional Electron Dynamics in the.
The Nature of the Pseudogap in Ultracold Fermi Gases Univ. of Washington May 2011.
From Local Moment to Mixed-Valence Regime in Ce 1−x Yb x CoIn 5 alloys Carmen Almasan, Kent State University, DMR Ce 1−x Yb x CoIn 5 alloys have.
Spatially resolved quasiparticle tunneling spectroscopic studies of cuprate and iron-based high-temperature superconductors Nai-Chang Yeh, California Institute.
Superconductivity and magnetism in organic materials Russell W. Giannetta, University of Illinois at Urbana-Champaign, DMR Our goal is to uncover.
It has long been recognized that the superconductors are intrinsically nonlinear. The investigation of their nonlinear behaviour might shed light into.
Non-Fermi liquid behavior with and without quantum criticality in Ce 1−x Yb x CoIn 5 Carmen C. Almasan, Kent State University, DMR One of the greatest.
Unconventional superconductivity, where Cooper pairing is driven by something other than electron-phonon coupling, often appears in proximity to magnetic.
6/7/2016 Iron Superconductivity !! o Superconducting Gap in FeAs from PCAR o “Minimal” Model of FeAs planes – Different from CuO 2 !! o Multiband Magnetism.
Superconductivity and Superfluidity The Microscopic Origins of Superconductivity The story so far -what do we know about superconductors?: (i) Superconductors.
New Materials and topological phases
ARPES studies of cuprates
High Temperature Superconductivity, Long-range Order and Broken Symmetries in Strongly Correlated Electronic Systems Lawrence J. Dunne , Erkki J. Brändas,
What is a quantum material?
CAN SUPERCONDUCTORS HELP WITH ENERGY AND ENVIRONMENTAL PROBLEMS?*
Toward a Holographic Model of d-wave Superconductors
BCS THEORY BCS theory is the first microscopic theory of superconductivity since its discovery in It explains, The interaction of phonons and electrons.
Electrical resistance
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
Giant Superconducting Proximity Effect in Composite Systems Chun Chen and Yan Chen Dept. of Physics and Lab of Advanced Materials, Fudan University,
Search of a Quantum Critical Point in High Tc Superconductors
Experimental Evidences on Spin-Charge Separation
Evidence for fully gapped superconductivity from microwave penetration depth measurements in PrFeAsO1-y single crystals K. Hashimoto1, T. Shibauchi1,
Magnetic, structural and electronic properties of LaFeAsO1-xFx
Bumsoo Kyung, Vasyl Hankevych, and André-Marie Tremblay
Phase diagram of s-wave SC Introduction
第38回応用物理学科セミナー 日時: 11月8日(水) 16:10 – 17:40 場所:葛飾キャンパス研究棟8F第1セミナー室
Quantum complexity in condensed matter physics
High Temperature Superconductivity
(Graduation thesis at Nihon University)
Aspects of Color Superconductivity in 2-flavor Quark Matter
Phases of Mott-Hubbard Bilayers Ref: Ribeiro et al, cond-mat/
Speaker:Prof. Kaori Tanaka
FSU Physics Department
Ginzburg-Landau theory
Presentation transcript:

第27回応用物理学科セミナー 日時: 10月25日(火) 16:00 – 17:30 場所:葛飾キャンパス研究棟8F第1セミナー室 Speaker:Prof. William Sacks, Affiliation: Sorbonne Universities, Paris Title:Pair-pair interactions in high-Tc superconductivity : evidence from tunneling experiments Abstract:  The conventional BCS theory fails to account for the physical properties of a large variety of high-Tc superconductors, the cuprate family and the recently discovered iron-based superconductors. In particular, these materials reveal a `peak-dip-hump' structure in the quasiparticle DOS at low temperature and often a pseudogap at the critical temperature. In my talk, the origin of these features are explained in the framework of a new pair-pair interaction model [1] : - The non-superconducting state consists of incoherent pairs, a `Cooper-pair glass' which, due to the pair-pair interaction, condense below Tc to the coherent superconducting state. - The peak-dip-hump structure is then due to the strong coupling between quasiparticles and excited pairs, which we call `super-quasiparticles'. The talk will focus on a wide variety of tunneling experiments, with varied temperature, magnetic field and doping, to test the validity of the model. [1] W. Sacks, A. Mauger, Y. Noat, Superconduct. Sci. Technol. 28 105014, (2015) 世話人:宮川 宣明