Principles of Electron Tunneling Spectroscopy
|
|
- Dwayne Thompson
- 5 years ago
- Views:
Transcription
1 Principles of Electron Tunneling Spectroscopy Second Edition E. L. Wolf Polytechnic Institute of New York University, USA OXFORD UNIVERSITY PRESS
2 Contents 1 Introduction 1.1 Concepts of quantum mechanical tunneling 1.2 Occurrence of tunneling phenomena 1.3 Electron tunneling in solid-state structures 1.4 Superconducting (quasipartide) and Josephson (pair) tunneling 1.5 Tunneling spectroscopies 1.6 The scanning tunneling microscope (STM): spectroscopic images 1.7 Atomic spatial resolution in the scanning tunneling microscope 1.8 Density of electron states (DOS) measurement in STM: STS 1.9 Perspective, scope, and organization 2 Tunneling in normal-state structures: I 2.1 Introduction 2.2 Calculational methods and models Stationary-state calculations Transfer Hamiltonian calculations Ideal barrier transmission 2.3 Basic junction types Metal-insulator-metal junctions Metal-insulator-semiconductor junctions Schottky barrier junctions pn junction (Esaki diode) direct case and the Si-Ge diode Vacuum tunneling Vacuum tunneling from a spherical STM tip 2.4 Dependence of J(V) and G(V) on band structure and density of states Fermi surface integrals Prefactors: wavefunction matching at boundaries 2.5 Nonideal barrier transmission Approach to ideal behavior Resonant barrier levels Two-step tunneling Barrier interactions 2.6 Assisted tunneling processes 2.7 Comments on the time for tunneling 2.8 Resolution obtained from a scanning tunneling microscope tip Tersoff and Hamann's model of STM resolution C. Julian Chen's atomic model of STM resolution 3 Spectroscopy of the superconducting energy gap: quasipartide and pair tunneling 3.1 Basic experiments of Giaever and Josephson tunneling 3.2 Superconductivity 3.3 Electron-phonon coupling and the BCS theory xi
3 3.3.1 The pair ground state Elementary excitations of superconductors Generalizations of BCS theory Theory of quasiparticle and pair tunneling Gap spectra of equilibrium BCS superconductors Gap spectra in more general homogeneous equilibrium superconductor cases Strong-coupling superconductors Gap anisotropy Multiple gaps, two-band superconductivity Excess currents, subharmonic structure Effects of magnetic field Magnetic impurities Pressure effects Interactions with electromagnetic radiation Superconducting fluctuations Ultrathin-film and small-particle superconductors Transition from tunnel junction to metallic contact Model of Klapwijk, Blonder, and Tinkham 171 Conventional tunneling spectroscopy of strong-coupling superconductors Introduction Eliashberg-Nambu strong-coupling theory of superconductivity Tunneling density of states Quantitative inversion for a 2 F(<w): test of Eliashberg theory Extension to more general cases Finite temperature Anisotropy Spin fluctuations Electronic density-of-states variation Limitations of the conventional method 194 Inhomogeneous superconductors: the superconducting proximity effect Introduction: continuity of the pair wavefunction Andreev reflection and specular SNS junctions Survey of phenomena in proximity tunneling structures Specular theory of tunneling into proximity structures McMillan's tunneling model of bilayers The Usadel equations and diffusive SNS junctions Reduction of Gor'kov's equations by Eilenberger and Usadel Application of reduced Gor'kov theory to tunneling problems The experiment of Truscott and Dynes confirming the bound state in clean NS junctions The experiment of le Sueur et al.: phase dependence of the density of states Proximity effects in a ferromagnetic N layer, in an NS structure Proximity electron tunneling spectroscopy (PETS) Effects of elastic scattering in the N layer Proximity corrections to conventional results Further applications of proximity effect models 251
4 xiii 6 Superconducting phonon spectra and a 2 F(co) Introduction s-p band elements Crystalline s-p band alloys and compounds Crystalline s-p band alloy superconductors s-p band compounds Amorphous metals Transition metals, alloys, and compounds Extreme weak-coupling metals Local-mode and resonance-mode superconductors Systematics of superconductivity Effects of external conditions and parameters on strong-coupling features Eliashberg inversion of bismuthate and cuprate superconductor tunneling data High-7^ electron-coupled superconductivity: cuprate and iron-based superconductors The discovery of cuprate superconductivity by Bednorz and Müller The Mott antiferromagnetic CuÜ2 insulator and its doping to a metal Paired holes in copper oxide planes Hubbard and t-j models in two dimensions Hole-doped cuprates Bi2212 and YBCO Phase diagram for superconductivity in hole-doped cuprate Crystal structures of common cuprates: I Early tunneling measurements on hole-doped superconductors Crystal structures of common cuprates: II Range of T c vs. number of copper oxide planes Disorder sites and doping of cuprate superconductors Comments on disorder and inhomogeneity in STS images Andreev-St. James tunneling spectroscopy Experimental signatures of nodal superconductivity Specific heat at transition Josephson junctions in d-wave cases Further examples of non-bcs superconductors Tunneling in normal-state structures: II Introduction Final-state effects: I Two-dimensional final states Quantum size effects in metal films Accumulation layers at semiconductor surfaces Spin-polarized tunneling as a probe of ferromagnets Julliere's model of ferromagnetic tunnel junctions Other bulk band structure effects Assisted tunneling: threshold spectroscopies Phonons Inelastic electron tunneling spectroscopy of molecular vibrations Inelastic excitations of spin waves (magnons) Inelastic excitation of surface and bulk plasmons Light emission by inelastic tunneling Spin-flip and Kondo scattering Excitation of electronic transitions 378
5 8.4 Final-state effects: II More general many-body theories of tunneling Tunneling studies of electron correlation and localization in metallic systems Phonon self-energy effects in degenerate semiconductors Electron scattering in the Kondo ground state Zero-bias anomalies Giant resistance peak Semiconductor conductance minima Assorted maxima and minima in metals The Giaever-Zeller resistance peak model Scanning tunneling spectroscopy (STS) of single atoms and molecules Theory of observation of single atoms in STS and experiment Friedel oscillations in 2-D surface state Effect of surface state: inference of wavevector Fourier-transform STM/STS Quantum corrals Elliptical corrals and focusing effects: quantum mirage Pair-breaking single adatoms on superconductors Mn and Cr on Pb Zn impurity atoms imaged in cuprate planes Spectroscopy of Kondo and spin-flip scattering Introduction Kondo spectroscopy of a single trapped electron Spectroscopy of localized moments in Si: As Schottky junctions Comparison of the two Kondo spectroscopy experiments STM spectroscopy of magnetic adatoms Molecules and their vibrational spectra Scanning tunneling spectroscopy of superconducting cuprates and magnetic manganites Gap imaging of optimally doped cuprates Site dependence of apparent gap Overdoped case Anticorrelation of gap and zero-bias density of states Internal proximity effect Localized state at Zn impurity Model for spectral distortions of noncuprate layers Superlattice modulation in Bi Fourier-transform STS (FT-STS) and application Observations of charge ordering in cuprate superconductors Relation of STS to angle-resolved photoemission spectroscopy (ARPES) Evidence for electron-spin wave coupling Colossal magnetoresistance: Mott transition in doped manganites Introduction: mechanism of colossal magnetoresistance (CMR) Pseudogap in manganite LSMO observed by ARPES Relation of cuprates to ferromagnetic CMR manganites Applications of barrier tunneling phenomena Introduction Josephson junction interferometers 477
6 11.3 SQUID detectors: the scanning SQUID microscope Establishing d-wave nature of cuprate pairing 11.4 Josephson junction logic: rapid single-flux quantum devices The single-flux quantum voltage pulse Analog to digital conversion (ADC) using RSFQ logic 11.5 Detection of radiation SIS detectors Josephson effect detectors Optical point-contact antennas (high-speed MIM junctions) 11.6 Tunnel-junction magnetoresistance sensors Appendix A Experimental methods of junction fabrication and characterization A. 1 Thin-film electrodes A. 1.1 Evaporated films A. 1.2 Film thickness measurement A. 1.3 Substrate temperature A. 1.4 Sputtered films A. 1.5 Chemical vapor-deposited films A. 1.6 Epitaxial single-crystal films A. 1.7 Atomic layer deposition A.2 Foil and single-crystal electrodes A.3 Characterization of tunneling electrodes A.4 Preparation of oxide tunneling barriers A.4.1 Thermal oxide barriers A.4.2 Plasma oxidation processes A.5 Artificial barriers A.5.1 Totally oxidized metal overlayers A.5.2 Directly deposited artificial barriers A.5.3 Polymerized organic films A.6 Point-contact barrier tunneling methods A.6.1 Anodized metal probes A.6.2 Schottky barrier probes A.6.3 Deformable metal vacuum tunneling probes A.6.4 Analysis of point-contact data A.7 Characterization of tunnel junctions A.7.1 Initial characterization of junctions A.7.2 Derivative measurement circuitry Appendix B Methods of scanning tunneling spectroscopy and competing approaches B.l STM basics, tip production, and characterization; single atom tips B.2 Noise-free x, y, z translation; vibration isolation B.2.1 The cryogenic STM of Wilson Ho B.2.2 The 240-mK STM design of Pan, Hudson, and J. C. Davis B.3 Atomic force microscope; combination STM/AFM B.4 Scanning tunneling potentiometry and point-contact measurements B.5 Ballistic electron emission microscopy (BEEM) B.6 Scanning charge microscopy and spectroscopy B.6.1 Scanning single-electron-transistor electrometry B.6.2 Scanning subsurface charge accumulation microscopy: STM/SCAM B.6.3 Single electron capacitance spectroscopy B.7 Scanning Hall probe microscopy
7 xvi CONTENTS Appendix C Tabulated results 542 Table C. 1 s, p elements 543 Table C.2 Alloys and unusual phases: s, p elements 544 Table C.3 d-band elements 545 Table C.4 d-band alloys, oxides, and compounds 546 Table C.5 f-band elements 548 Table C.6 Metal overlayers for barrier formation 548 Table C.7 Studies of Tomasch oscillations in thick superconducting films Table C.8 and of McMillan-Rowell oscillations in thick normal films 548 Tunneling studies of superconductor phonons under hydrostatic pressure 548 Tables C.9 Cuprate superconductors 549 Table C.9a Gap values for Bi 2 Sr2CaCu ( s (Bi2212) 549 Table C.9b Gap values for YBa 2 Cu30 7+,5 550 Table C.9c Gap values for HgBa2Ca _icu n 02 n +2+,5 551 References 553 Index 583
Solid Surfaces, Interfaces and Thin Films
Hans Lüth Solid Surfaces, Interfaces and Thin Films Fifth Edition With 427 Figures.2e Springer Contents 1 Surface and Interface Physics: Its Definition and Importance... 1 Panel I: Ultrahigh Vacuum (UHV)
More informationSOLID STATE PHYSICS. Second Edition. John Wiley & Sons. J. R. Hook H. E. Hall. Department of Physics, University of Manchester
SOLID STATE PHYSICS Second Edition J. R. Hook H. E. Hall Department of Physics, University of Manchester John Wiley & Sons CHICHESTER NEW YORK BRISBANE TORONTO SINGAPORE Contents Flow diagram Inside front
More informationINTRODUCTION TO SCA\ \I\G TUNNELING MICROSCOPY
INTRODUCTION TO SCA\ \I\G TUNNELING MICROSCOPY SECOND EDITION C. JULIAN CHEN Department of Applied Physics and Applied Mathematics, Columbia University, New York OXFORD UNIVERSITY PRESS Contents Preface
More informationOptical Characterization of Solids
D. Dragoman M. Dragoman Optical Characterization of Solids With 184 Figures Springer 1. Elementary Excitations in Solids 1 1.1 Energy Band Structure in Crystalline Materials 2 1.2 k p Method 11 1.3 Numerical
More informationConcepts in Surface Physics
M.-C. Desjonqueres D. Spanjaard Concepts in Surface Physics Second Edition With 257 Figures Springer 1. Introduction................................. 1 2. Thermodynamical and Statistical Properties of
More informationScanning Tunneling Spectroscopy Studies of High-Temperature Cuprate Superconductors
Scanning Tunneling Spectroscopy Studies of High-Temperature Cuprate Superconductors Thesis by Ching-Tzu Chen In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy California
More informationChapter 5 Nanomanipulation. Chapter 5 Nanomanipulation. 5.1: With a nanotube. Cutting a nanotube. Moving a nanotube
Objective: learn about nano-manipulation techniques with a STM or an AFM. 5.1: With a nanotube Moving a nanotube Cutting a nanotube Images at large distance At small distance : push the NT Voltage pulse
More informationConductor Insulator Quantum
Conductor Insulator Quantum Phase Transitions Edited by Vladimir Dobrosavljevic, Nandini Trivedi, James M. Valles, Jr. OXPORD UNIVERSITY PRESS Contents List of abbreviations List of contributors xiv xvi
More informationTunneling Spectra of Hole-Doped YBa 2 Cu 3 O 6+δ
67 Chapter 4 Tunneling Spectra of Hole-Doped YBa 2 Cu 3 O 6+δ 1 4.1 Introduction The proximity of cuprate superconductors to the Mott insulating phase gives rise to novel superconducting behavior enriched
More informationMetals: the Drude and Sommerfeld models p. 1 Introduction p. 1 What do we know about metals? p. 1 The Drude model p. 2 Assumptions p.
Metals: the Drude and Sommerfeld models p. 1 Introduction p. 1 What do we know about metals? p. 1 The Drude model p. 2 Assumptions p. 2 The relaxation-time approximation p. 3 The failure of the Drude model
More informationThe Physics of Nanoelectronics
The Physics of Nanoelectronics Transport and Fluctuation Phenomena at Low Temperatures Tero T. Heikkilä Low Temperature Laboratory, Aalto University, Finland OXFORD UNIVERSITY PRESS Contents List of symbols
More informationTransport through Andreev Bound States in a Superconductor-Quantum Dot-Graphene System
Transport through Andreev Bound States in a Superconductor-Quantum Dot-Graphene System Nadya Mason Travis Dirk, Yung-Fu Chen, Cesar Chialvo Taylor Hughes, Siddhartha Lal, Bruno Uchoa Paul Goldbart University
More informationTwenty years have passed since the discovery of the first copper-oxide high-temperature superconductor
1 Chapter 1 Introduction Twenty years have passed since the discovery of the first copper-oxide high-temperature superconductor La 2 x Ba x CuO 4 in 1986, and the intriguing physics of cuprate superconductors
More informationElectronic and Optoelectronic Properties of Semiconductor Structures
Electronic and Optoelectronic Properties of Semiconductor Structures Jasprit Singh University of Michigan, Ann Arbor CAMBRIDGE UNIVERSITY PRESS CONTENTS PREFACE INTRODUCTION xiii xiv 1.1 SURVEY OF ADVANCES
More informationImpact of disorder and topology in two dimensional systems at low carrier densities
Impact of disorder and topology in two dimensional systems at low carrier densities A Thesis Submitted For the Degree of Doctor of Philosophy in the Faculty of Science by Mohammed Ali Aamir Department
More information2 Metallic point contacts as a physical tool
2 Metallic point contacts as a physical tool Already more than 100 years ago Drude developed a theory for the electrical and thermal conduction of metals based on the classic kinetic theory of gases. Drude
More informationMagnetism in correlated-electron materials
Magnetism in correlated-electron materials B. Keimer Max-Planck-Institute for Solid State Research focus on delocalized electrons in metals and superconductors localized electrons: Hinkov talk outline
More informationrequires going beyond BCS theory to include inelastic scattering In conventional superconductors we use Eliashberg theory to include the electron-
MECHANISM requires going beyond BCS theory to include inelastic scattering In conventional superconductors we use Eliashberg theory to include the electron- A serious limitation of BCS theory is that it
More informationTime-Resolved and Momentum-Resolved Resonant Soft X-ray Scattering on Strongly Correlated Systems
Time-Resolved and Momentum-Resolved Resonant Soft X-ray Scattering on Strongly Correlated Systems Wei-Sheng Lee Stanford Institute of Material and Energy Science (SIMES) SLAC & Stanford University Collaborators
More informationSTM spectroscopy (STS)
STM spectroscopy (STS) di dv 4 e ( E ev, r) ( E ) M S F T F Basic concepts of STS. With the feedback circuit open the variation of the tunneling current due to the application of a small oscillating voltage
More information2) Atom manipulation. Xe / Ni(110) Model: Experiment:
2) Atom manipulation D. Eigler & E. Schweizer, Nature 344, 524 (1990) Xe / Ni(110) Model: Experiment: G.Meyer, et al. Applied Physics A 68, 125 (1999) First the tip is approached close to the adsorbate
More informationElectronic Noise Due to Thermal Stripe Switching
Electronic Noise Due to Thermal Stripe Switching E. W. Carlson B. Phillabaum Y. L. Loh D. X. Yao Research Corporation Solid Liquid Gas www.stonecropgallery.com/artists/caleb/01-solidliquidgas.jpg Crystals
More informationHarald Ibach Hans Lüth SOLID-STATE PHYSICS. An Introduction to Theory and Experiment
Harald Ibach Hans Lüth SOLID-STATE PHYSICS An Introduction to Theory and Experiment With 230 Figures Springer-Verlag Berlin Heidelberg New York London Paris Tokyo Hong Kong Barcelona Budapest Contents
More informationSemiconductor Physical Electronics
Semiconductor Physical Electronics Sheng S. Li Department of Electrical Engineering University of Florida Gainesville, Florida Plenum Press New York and London Contents CHAPTER 1. Classification of Solids
More informationVibrational Spectroscopy of Molecules on Surfaces
Vibrational Spectroscopy of Molecules on Surfaces Edited by John T. Yates, Jr. University of Pittsburgh Pittsburgh, Pennsylvania and Theodore E. Madey National Bureau of Standards Gaithersburg, Maryland
More informationWhat's so unusual about high temperature superconductors? UBC 2005
What's so unusual about high temperature superconductors? UBC 2005 Everything... 1. Normal State - doped Mott insulator 2. Pairing Symmetry - d-wave 2. Short Coherence Length - superconducting fluctuations
More informationSheng S. Li. Semiconductor Physical Electronics. Second Edition. With 230 Figures. 4) Springer
Sheng S. Li Semiconductor Physical Electronics Second Edition With 230 Figures 4) Springer Contents Preface 1. Classification of Solids and Crystal Structure 1 1.1 Introduction 1 1.2 The Bravais Lattice
More informationsingle-electron electron tunneling (SET)
single-electron electron tunneling (SET) classical dots (SET islands): level spacing is NOT important; only the charging energy (=classical effect, many electrons on the island) quantum dots: : level spacing
More informationNeutron scattering from quantum materials
Neutron scattering from quantum materials Bernhard Keimer Max Planck Institute for Solid State Research Max Planck UBC UTokyo Center for Quantum Materials Detection of bosonic elementary excitations in
More information3.1 Electron tunneling theory
Scanning Tunneling Microscope (STM) was invented in the 80s by two physicists: G. Binnig and H. Rorher. They got the Nobel Prize a few years later. This invention paved the way for new possibilities in
More informationTheory of Nonequilibrium Superconductivity *
Theory of Nonequilibrium Superconductivity * NIKOLAI B.KOPNIN Low Temperature Laboratory, Helsinki University of Technology, Finland and L.D. Landau Institute for Theoretical Physics, Moscow, Russia CLARENDON
More informationEffective masses in semiconductors
Effective masses in semiconductors The effective mass is defined as: In a solid, the electron (hole) effective mass represents how electrons move in an applied field. The effective mass reflects the inverse
More informationThe Oxford Solid State Basics
The Oxford Solid State Basics Steven H. Simon University of Oxford OXFORD UNIVERSITY PRESS Contents 1 About Condensed Matter Physics 1 1.1 What Is Condensed Matter Physics 1 1.2 Why Do We Study Condensed
More informationTuning order in cuprate superconductors
Tuning order in cuprate superconductors arxiv:cond-mat/0201401 v1 23 Jan 2002 Subir Sachdev 1 and Shou-Cheng Zhang 2 1 Department of Physics, Yale University, P.O. Box 208120, New Haven, CT 06520-8120,
More informationSolid State Physics. GIUSEPPE GROSSO Professor of Solid State Physics, Department of Physics, University of Pavia, and INFM
Solid State Physics GIUSEPPE GROSSO Professor of Solid State Physics, Department of Physics, University of Pisa, and INFM GIUSEPPE PASTORI PARRAVICINI Professor of Solid State Physics, Department of Physics,
More informationMetal-Insulator Transitions
Metal-Insulator Transitions Second Edition N. F. MOTT Emeritus Cavendish Professor of Physics University of Cambridge Taylor & Francis London New York Philadelphia Contents Preface to Second Edition v
More informationSpectroscopy at nanometer scale
Spectroscopy at nanometer scale 1. Physics of the spectroscopies 2. Spectroscopies for the bulk materials 3. Experimental setups for the spectroscopies 4. Physics and Chemistry of nanomaterials Various
More informationVisualization of atomic-scale phenomena in superconductors
Visualization of atomic-scale phenomena in superconductors Andreas Kreisel, Brian Andersen Niels Bohr Institute, University of Copenhagen, 2100 København, Denmark Peayush Choubey, Peter Hirschfeld Department
More informationElectron State and Lattice Effects in Cuprate High Temperature Superconductors
Electron State and Lattice Effects in Cuprate High Temperature Superconductors - The True Story Revealed by Fermi Surface and Unconventional Lattice Effects- October 27-28, 2005 Headquarters and Information
More informationPhysics of Low-Dimensional Semiconductor Structures
Physics of Low-Dimensional Semiconductor Structures Edited by Paul Butcher University of Warwick Coventry, England Norman H. March University of Oxford Oxford, England and Mario P. Tosi Scuola Normale
More informationScanning Tunneling Microscopy and its Application
Chunli Bai Scanning Tunneling Microscopy and its Application With 181 Figures SHANGHAI SCIENTIFIC & TECHNICAL PUBLISHERS Jpl Springer Contents 1. Introduction 1 1.1 Advantages of STM Compared with Other
More informationVortex Checkerboard. Chapter Low-T c and Cuprate Vortex Phenomenology
63 Chapter 4 Vortex Checkerboard There is no need to invoke alternative order parameters to explain observed DOS modulations in optimally doped Bi 2 Sr 2 CaCu 2 O 8+δ. To continue the search for interesting
More informationQuantum Condensed Matter Physics Lecture 12
Quantum Condensed Matter Physics Lecture 12 David Ritchie QCMP Lent/Easter 2016 http://www.sp.phy.cam.ac.uk/drp2/home 12.1 QCMP Course Contents 1. Classical models for electrons in solids 2. Sommerfeld
More informationCan superconductivity emerge out of a non Fermi liquid.
Can superconductivity emerge out of a non Fermi liquid. Andrey Chubukov University of Wisconsin Washington University, January 29, 2003 Superconductivity Kamerling Onnes, 1911 Ideal diamagnetism High Tc
More informationNeutron and x-ray spectroscopy
Neutron and x-ray spectroscopy B. Keimer Max-Planck-Institute for Solid State Research outline 1. self-contained introduction neutron scattering and spectroscopy x-ray scattering and spectroscopy 2. application
More informationMaterial Science II. d Electron systems
Material Science II. d Electron systems 1. Electronic structure of transition-metal ions (May 23) 2. Crystal structure and band structure (June 13) 3. Mott s (June 20) 4. Metal- transition (June 27) 5.
More informationIntroduction to Superconductivity. Superconductivity was discovered in 1911 by Kamerlingh Onnes. Zero electrical resistance
Introduction to Superconductivity Superconductivity was discovered in 1911 by Kamerlingh Onnes. Zero electrical resistance Meissner Effect Magnetic field expelled. Superconducting surface current ensures
More informationOPTICAL PROPERTIES AND SPECTROSCOPY OF NANOAAATERIALS. Jin Zhong Zhang. World Scientific TECHNISCHE INFORMATIONSBIBLIOTHEK
OPTICAL PROPERTIES AND SPECTROSCOPY OF NANOAAATERIALS Jin Zhong Zhang University of California, Santa Cruz, USA TECHNISCHE INFORMATIONSBIBLIOTHEK Y World Scientific NEW JERSEY. t'on.don SINGAPORE «'BEIJING
More information(a) (b) Supplementary Figure 1. (a) (b) (a) Supplementary Figure 2. (a) (b) (c) (d) (e)
(a) (b) Supplementary Figure 1. (a) An AFM image of the device after the formation of the contact electrodes and the top gate dielectric Al 2 O 3. (b) A line scan performed along the white dashed line
More informationElectronic Quantum Transport in Mesoscopic Semiconductor Structures
Thomas Ihn Electronic Quantum Transport in Mesoscopic Semiconductor Structures With 90 Illustrations, S in Full Color Springer Contents Part I Introduction to Electron Transport l Electrical conductance
More informationModern Physics for Scientists and Engineers International Edition, 4th Edition
Modern Physics for Scientists and Engineers International Edition, 4th Edition http://optics.hanyang.ac.kr/~shsong 1. THE BIRTH OF MODERN PHYSICS 2. SPECIAL THEORY OF RELATIVITY 3. THE EXPERIMENTAL BASIS
More informationC. R. Hughes, 1 J. Shi, 1 A. D. Beyer, 1 and N.-C. Yeh 2,1
Spin-polarized tunneling spectroscopic studies of the intrinsic heterogeneity and pseudogap phenomena in colossal magnetoresistive manganite La 0.7 Ca 0.3 MnO 3 C. R. Hughes, 1 J. Shi, 1 A. D. Beyer, 1
More informationQuantum Tunneling and
BEIJING SHANGHAI Quantum Tunneling and Field Electron Emission Theories Shi-Dong Liang Sun Yat-Sen University, China World Scientific NEW JERSEY LONDON SINGAPORE HONG KONG TAIPEI CHENNAI Contents Preface
More informationMicroscopical and Microanalytical Methods (NANO3)
Microscopical and Microanalytical Methods (NANO3) 06.11.15 10:15-12:00 Introduction - SPM methods 13.11.15 10:15-12:00 STM 20.11.15 10:15-12:00 STS Erik Zupanič erik.zupanic@ijs.si stm.ijs.si 27.11.15
More informationSuperconducting Stripes
Superconducting Stripes By: Nick Vence I. Introduction In 1972 Bardeen, Cooper, and Schrieffer shared the Nobel prize in physics for describing a mechanism of superconductivity. Their BCS theory describes
More informationSuperconductivity. S2634: Physique de la matière condensée & nano-objets. Miguel Anía Asenjo Alexandre Le Boité Christine Lingblom
Superconductivity S2634: Physique de la matière condensée & nano-objets Miguel Anía Asenjo Alexandre Le Boité Christine Lingblom 1 What is superconductivity? 2 Superconductivity Superconductivity generally
More informationStrongly Correlated Systems:
M.N.Kiselev Strongly Correlated Systems: High Temperature Superconductors Heavy Fermion Compounds Organic materials 1 Strongly Correlated Systems: High Temperature Superconductors 2 Superconductivity:
More informationElectronic Properties of Materials An Introduction for Engineers
Rolf E. Hummel Electronic Properties of Materials An Introduction for Engineers With 219 Illustrations Springer-Verlag Berlin Heidelberg New York Tokyo Contents PARTI Fundamentals of Electron Theory CHAPTER
More informationIntroduction to Scanning Tunneling Microscopy
Introduction to Scanning Tunneling Microscopy C. JULIAN CHEN IBM Research Division Thomas J. Watson Research Center Yorktown Heights, New York New York Oxford OXFORD UNIVERSITY PRESS 1993 CONTENTS List
More informationMolecules and Condensed Matter
Chapter 42 Molecules and Condensed Matter PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Goals for Chapter 42 To understand
More informationCorrelated 2D Electron Aspects of the Quantum Hall Effect
Correlated 2D Electron Aspects of the Quantum Hall Effect Magnetic field spectrum of the correlated 2D electron system: Electron interactions lead to a range of manifestations 10? = 4? = 2 Resistance (arb.
More informationChapter 103 Spin-Polarized Scanning Tunneling Microscopy
Chapter 103 Spin-Polarized Scanning Tunneling Microscopy Toyo Kazu Yamada Keywords Spin-polarized tunneling current Spin polarization Magnetism 103.1 Principle Spin-polarized scanning tunneling microscopy
More informationMODERN PHYSICS Frank J. Blatt Professor of Physics, University of Vermont
MODERN PHYSICS Frank J. Blatt Professor of Physics, University of Vermont McGRAW-HILL, INC. New York St. Louis San Francisco Auckland Bogota Caracas Lisbon London Madrid Mexico Milan Montreal New Delhi
More informationModeling Schottky barrier SINIS junctions
Modeling Schottky barrier SINIS junctions J. K. Freericks, B. Nikolić, and P. Miller * Department of Physics, Georgetown University, Washington, DC 20057 * Department of Physics, Brandeis University, Waltham,
More informationHigh temperature superconductivity
High temperature superconductivity Applications to the maglev industry Elsa Abreu April 30, 2009 Outline Historical overview of superconductivity Copper oxide high temperature superconductors Angle Resolved
More informationSupplementary figures
Supplementary figures Supplementary Figure 1. A, Schematic of a Au/SRO113/SRO214 junction. A 15-nm thick SRO113 layer was etched along with 30-nm thick SRO214 substrate layer. To isolate the top Au electrodes
More informationSuperconducting fluctuations, interactions and disorder : a subtle alchemy
Les défis actuels de la supraconductivité Dautreppe 2011 Superconducting fluctuations, interactions and disorder : a subtle alchemy Claude Chapelier, Benjamin Sacépé, Thomas Dubouchet INAC-SPSMS-LaTEQS,
More informationDynamics of fluctuations in high temperature superconductors far from equilibrium. L. Perfetti, Laboratoire des Solides Irradiés, Ecole Polytechnique
Dynamics of fluctuations in high temperature superconductors far from equilibrium L. Perfetti, Laboratoire des Solides Irradiés, Ecole Polytechnique Superconductors display amazing properties: Dissipation-less
More informationSpectroscopy of Nanostructures. Angle-resolved Photoemission (ARPES, UPS)
Spectroscopy of Nanostructures Angle-resolved Photoemission (ARPES, UPS) Measures all quantum numbers of an electron in a solid. E, k x,y, z, point group, spin E kin, ϑ,ϕ, hν, polarization, spin Electron
More information1.9.5 Stoichiometry, Nonstoichiometry, and Defect Structures 75
Chapter 1 Elementary Materials Science Concepts 3 1.1 Atomic Structure and Atomic Number 3 1.2 Atomic Mass and Mole 8 1.3 Bonding and Types of Solids 9 1.3.1 Molecules and General Bonding Principles 9
More informationScanning Tunneling Microscopy. how does STM work? the quantum mechanical picture example of images how can we understand what we see?
Scanning Tunneling Microscopy how does STM work? the quantum mechanical picture example of images how can we understand what we see? Observation of adatom diffusion with a field ion microscope Scanning
More informationHigh-Temperature Superconductors: Playgrounds for Broken Symmetries
High-Temperature Superconductors: Playgrounds for Broken Symmetries Gauge / Phase Reflection Time Laura H. Greene Department of Physics Frederick Seitz Materials Research Laboratory Center for Nanoscale
More informationAdvanced Spectroscopies of Modern Quantum Materials
Advanced Spectroscopies of Modern Quantum Materials The part about Advanced spectroscopies Some course goals: Better understand the link between experiment and the microscopic world of quantum materials.
More informationScanning Tunnelling Microscopy Observations of Superconductivity
Department of physics Seminar I a Scanning Tunnelling Microscopy Observations of Superconductivity Author: Tim Verbovšek Mentor: dr. Rok Žitko Co-Mentor: dr. Erik Zupanič Ljubljana, February 013 Abstract
More informationMAGNETORESISTANCE PHENOMENA IN MAGNETIC MATERIALS AND DEVICES. J. M. De Teresa
MAGNETORESISTANCE PHENOMENA IN MAGNETIC MATERIALS AND DEVICES J. M. De Teresa Instituto de Ciencia de Materiales de Aragón, Universidad de Zaragoza-CSIC, Facultad de Ciencias, 50009 Zaragoza, Spain. E-mail:
More informationFoundations of Condensed Matter Physics
Foundations of Condensed Matter Physics PHY1850F 2005 www.physics.utoronto.ca/~wei/phy1850f.html Physics 1850F Foundations of Condensed Matter Physics Webpage: www.physics.utoronto.ca/~wei/phy1850f.html
More informationQUESTIONS AND ANSWERS
QUESTIONS AND ANSWERS (1) For a ground - state neutral atom with 13 protons, describe (a) Which element this is (b) The quantum numbers, n, and l of the inner two core electrons (c) The stationary state
More informationLecture 2. Introduction to semiconductors Structures and characteristics in semiconductors. Fabrication of semiconductor sensor
Lecture 2 Introduction to semiconductors Structures and characteristics in semiconductors Semiconductor p-n junction Metal Oxide Silicon structure Semiconductor contact Fabrication of semiconductor sensor
More informationChapter 2. Theoretical background. 2.1 Itinerant ferromagnets and antiferromagnets
Chapter 2 Theoretical background The first part of this chapter gives an overview of the main static magnetic behavior of itinerant ferromagnetic and antiferromagnetic materials. The formation of the magnetic
More informationedited by Nan-Lin Wang Hideo Hosono Pengcheng Dai MATERIALS, PROPERTIES, AND MECHANISMS IRON-BASED SUPERCONDUCTORS
edited by " Nan-Lin Wang Hideo Hosono Pengcheng Dai MATERIALS, PROPERTIES, AND MECHANISMS IRON-BASED SUPERCONDUCTORS Pan Stanford Publishing Contents Preface xiii 1 Iron-Based Superconductors: Discovery
More informationTuning a short coherence length Josephson junction through a metal-insulator transition
Tuning a short coherence length Josephson junction through a metal-insulator transition J. K. Freericks, B. Nikolić, and P. Miller * Department of Physics, Georgetown University, Washington, DC 20057 *
More informationTunneling Spectroscopy of PCCO
Tunneling Spectroscopy of PCCO Neesha Anderson and Amlan Biswas Department of Physics, University of Florida, Gainesville, Florida Abstract A point-contact probe capable of operating down to temperatures
More informationQuantum dynamics in many body systems
Quantum dynamics in many body systems Eugene Demler Harvard University Collaborators: David Benjamin (Harvard), Israel Klich (U. Virginia), D. Abanin (Perimeter), K. Agarwal (Harvard), E. Dalla Torre (Harvard)
More informationMODERN TECHNIQUES OF SURFACE SCIENCE
MODERN TECHNIQUES OF SURFACE SCIENCE Second edition D. P. WOODRUFF & T. A. DELCHAR Department ofphysics, University of Warwick CAMBRIDGE UNIVERSITY PRESS Contents Preface to first edition Preface to second
More informationClassification of Solids
Classification of Solids Classification by conductivity, which is related to the band structure: (Filled bands are shown dark; D(E) = Density of states) Class Electron Density Density of States D(E) Examples
More informationSemiconductor Detectors
Semiconductor Detectors Summary of Last Lecture Band structure in Solids: Conduction band Conduction band thermal conductivity: E g > 5 ev Valence band Insulator Charge carrier in conductor: e - Charge
More informationConcepts in Spin Electronics
Concepts in Spin Electronics Edited by Sadamichi Maekawa Institutefor Materials Research, Tohoku University, Japan OXFORD UNIVERSITY PRESS Contents List of Contributors xiii 1 Optical phenomena in magnetic
More informationCitation PHYSICAL REVIEW LETTERS (2000), 85( RightCopyright 2000 American Physical So
Title Discriminating the superconducting Bi2Sr2CaCu2O8+delta by interlayer t Author(s) Suzuki, M; Watanabe, T Citation PHYSICAL REVIEW LETTERS (2), 85( Issue Date 2-11-27 URL http://hdl.handle.net/2433/39919
More informationPhotoelectron Spectroscopy
Stefan Hüfner Photoelectron Spectroscopy Principles and Applications Third Revised and Enlarged Edition With 461 Figures and 28 Tables JSJ Springer ... 1. Introduction and Basic Principles 1 1.1 Historical
More informationCrossover from phase fluctuation to amplitudedominated superconductivity: A model system
Santa Clara University Scholar Commons Physics College of Arts & Sciences 3-6-2001 Crossover from phase fluctuation to amplitudedominated superconductivity: A model system Richard P. Barber Jr. Santa Clara
More informationSuperconducting Single-photon Detectors
: Quantum Cryptography Superconducting Single-photon Detectors Hiroyuki Shibata Abstract This article describes the fabrication and properties of a single-photon detector made of a superconducting NbN
More informationSemiconductors and Optoelectronics. Today Semiconductors Acoustics. Tomorrow Come to CH325 Exercises Tours
Semiconductors and Optoelectronics Advanced Physics Lab, PHYS 3600 Don Heiman, Northeastern University, 2017 Today Semiconductors Acoustics Tomorrow Come to CH325 Exercises Tours Semiconductors and Optoelectronics
More informationIntrinsic tunnelling data for Bi-2212 mesa structures and implications for other properties.
Intrinsic tunnelling data for Bi-2212 mesa structures and implications for other properties. J.R. Cooper, QM group, Cavendish Laboratory, University of Cambridge, Cambridge CB3 0HE, UK e-mail jrc19@cam.ac.uk
More informationMinimal Update of Solid State Physics
Minimal Update of Solid State Physics It is expected that participants are acquainted with basics of solid state physics. Therefore here we will refresh only those aspects, which are absolutely necessary
More informationArtificially layered structures
http://accessscience.com/popup.ap x?id=053450&name=print Close Window ENCYCLOPEDIA ARTICLE Artificially layered structures Manufactured, reproducibly layered structures having layer thicknesses approaching
More informationEE 3329 Electronic Devices Syllabus ( Extended Play )
EE 3329 - Electronic Devices Syllabus EE 3329 Electronic Devices Syllabus ( Extended Play ) The University of Texas at El Paso The following concepts can be part of the syllabus for the Electronic Devices
More informationQuantum Theory of Matter
Quantum Theory of Matter Overview Lecture Derek Lee Imperial College London January 2007 Outline 1 Course content Introduction Superfluids Superconductors 2 Course Plan Resources Outline 1 Course content
More informationStripes developed at the strong limit of nematicity in FeSe film
Stripes developed at the strong limit of nematicity in FeSe film Wei Li ( ) Department of Physics, Tsinghua University IASTU Seminar, Sep. 19, 2017 Acknowledgements Tsinghua University Prof. Qi-Kun Xue,
More informationHerre van der Zant. interplay between molecular spin and electron transport (molecular spintronics) Gate
transport through the single molecule magnet Mn12 Herre van der Zant H.B. Heersche, Z. de Groot (Delft) C. Romeike, M. Wegewijs (RWTH Aachen) D. Barreca, E. Tondello (Padova) L. Zobbi, A. Cornia (Modena)
More informationHigh-temperature superconductivity
Superconductivity and Low temperature physics, FMI036 High-temperature superconductivity Alexey Kalabukhov Quantum Device Physics Laboratory, MC2 Outline Lecture I (19/2): History of discovery, phenomenology
More information