If a 2D metal, also known as a quantum Hall system (QHS), is cooled down to not-too-low temperature, its electrical properties are strongly influenced.

Slides:



Advertisements
Similar presentations
Single Electron Devices Single-electron Transistors
Advertisements

Atom Chip Technology (ACT) A New Program to Focus a New Quantum Technology for Emerging National Needs CQI Please See Nick Bigelow With Questions.
Early Quantum Theory and Models of the Atom
Quantum Hall effect at with light John Cerne, SUNY at Buffalo, DMR In metals, magnetic fields deflect moving charges to produce an electric field.
ECE 875: Electronic Devices Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University
Carrier Transport Phenomena
World of ultracold atoms with strong interaction National Tsing-Hua University Daw-Wei Wang.
World of zero temperature --- introduction to systems of ultracold atoms National Tsing-Hua University Daw-Wei Wang.
1 Chapter 27 Current and Resistance. 2 Electric Current Electric current is the rate of flow of charge through some region of space The SI unit of current.
Dynamics of Quantal Heating in Electron Systems with Discrete Spectra William Mayer 1,2, S. Dietrich 1,2, S. Vitkalov 1, A. A. Bykov 3,4 1. City College.
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
M V V K Srinivas Prasad K L University.  Ohm’s Law ◦ At constant temperature the current flowing through a conductor is directly proportional to the.
Answers to Questions from Lecture 4 Q1: How old is the cyclotron resonance method of determining the effective mass of electrons and holes in semiconductors?
Mott Transition, i.e., the interaction-driven metal-to- insulator transition (MIT), is a fundamental issue in the physics of strongly correlated electron.
Current and Direct Current Circuits
Computational Solid State Physics 計算物性学特論 第9回 9. Transport properties I: Diffusive transport.
Superconducting/Semiconducting Nanowires, Nanotubes, and Ultrathin Films Wenhao Wu, Texas A&M University, DMR We use membranes with a honeycomb.
Slide # 1 SPM Probe tips CNT attached to a Si probe tip.
Frequency dependence of the anomalous Hall effect: possible transition from extrinsic to intrinsic behavior John Cerne, University at Buffalo, SUNY, DMR.
National Science Foundation Material for Future Low-Power Electronics Daniel Gall, Rensselaer Polytechnic Institute, DMR Outcome: Researchers at.
Chapter 34 Electromagnetic Waves. Currents produce B Change in E produces B Currents produce B Change in E produces B Change in B produces an E charges.
Strands of DNA have been used as tiny scaffolds to create superconducting nanodevices that demonstrate a new quantum interference phenomenon. These nanowire.
Electrical Conduction in Solids
Electro-Optic Studies of Charge Density Wave Conductors Joseph W. Brill, University of Kentucky, DMR One-dimensional charge-density-wave (CDW)
NDR & The Gunn Effect. For direct bandgap materials, like GaAs: v d vs. E peaks before saturation & decreases again, after which it finally saturates.
Using quantum-well “nano-apertures” to probe hot-electron motion in metal films Jonathan Pelz, Ohio State University, DMR Unique cleaved-quantum.
Specific Heat of Solids Quantum Size Effect on the Specific Heat Electrical and Thermal Conductivities of Solids Thermoelectricity Classical Size Effect.
Lecture 4 OUTLINE Semiconductor Fundamentals (cont’d)
Zero electrical resistance is a rare occurrence in condensed matter physics, with superconductivity and quantum Hall effect being prime examples. However,
The discovery of the fractional quantum Hall state at the quantum number 5/2 has reinvigorated studies of the two-dimensional electron gas. The prediction.
Chap. 41: Conduction of electricity in solids Hyun-Woo Lee.
Infrared Hall effect in conventional and unconventional materials John Cerne, SUNY at Buffalo, DMR In metals, magnetic fields (H) deflect moving.
Michael Browne 11/26/2007.
Review Warm Up 1.An object is dropped from rest from a height of 12 meters above the ground. The object falls freely and reaches the ground 1.1 seconds.
High E Field Transport BW: Sect. 8.10, p 198YC, Sect. 5.4; S, Sect. 4.13; + Outside sources.
Jean Baptiste Perrin Nobel Prize in physics 1926 He demonstrated that the current in a vacuum tube was due to electron motion.
Anomalous correlated electron phenomena in Yb 2 Fe 12 P 7 M. Brian Maple, University of California-San Diego, DMR Temperature – magnetic field.
Magnetothermopower in high-mobility 2D electron gas: effect of microwave irradiation Oleg Raichev Department of Theoretical Physics Institute of Semiconductor.
Chapter 26 Lecture 22: Current: II
Chapter 27 Current and Resistance. Electrical Conduction – A Model Treat a conductor as a regular array of atoms plus a collection of free electrons.
Dr. Nasim Zafar Electronics 1 EEE 231 – BS Electrical Engineering Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Phonons Packets of sound found present in the lattice as it vibrates … but the lattice vibration cannot be heard. Unlike static lattice model , which.
Sid Nb device fabrication Superconducting Nb thin film evaporation Evaporate pure Nb to GaAs wafer and test its superconductivity (T c ~9.25k ) Tc~2.5K.
Quantum transport in one and two dimensional superconductors Andrey Rogachev, University of Utah, DMR Superconductor-Insulator Transition in 1D.
Dynamics of Localized Photoexcitations in Condensed Matter Systems Susan L. Dexheimer, Washington State University, DMR Localization of electronic.
A.A. Bykov, I.S. Strygin, D.V. Dmitriev
Quantum Criticality in Magnetic Single-Electron Transistors T p Physics of non-Fermi-liquid Metals Qimiao Si, Rice University, DMR Quantum criticality.
Magnetic Moments in Amorphous Semiconductors Frances Hellman, University of California, Berkeley, DMR This project looks at the effect of magnetic.
Waves, Light, and the EM Spectrum ● What is a wave? ● What are the main properties of waves? ● What two things do all waves transport?
Magnetotransport Studies of Organic Spin Valves A. M. Goldman, University of Minnesota, DMR Graph of the resistance versus magnetic field at 100K.
Secondary Electron Emission in the Limit of Low Energy and its Effect on High Energy Physics Accelerators A. N. ANDRONOV, A. S. SMIRNOV, St. Petersburg.
Energy Gaps Insulators & Superconductors When does an energy or band gap lead to insulating behavior? Band gap insulators, Peierls’ insulators When does.
Professor Philip Burrows John Adams Institute for Accelerator Science Oxford University ACAS School for Accelerator Physics January 2014 Longitudinal Dynamics.
Nanoelectronics Part II Many Electron Phenomena Chapter 10 Nanowires, Ballistic Transport, and Spin Transport
Phonons Packets of sound found present in the lattice as it vibrates … but the lattice vibration cannot be heard. Unlike static lattice model, which deals.
Matching: 1. Insulator 2. Positive 3. Ion 4. Negative 5. Conductor 6. Electricity A. The charge that attracts electrons. B. An atom with a different number.
Lecture 4 OUTLINE Semiconductor Fundamentals (cont’d)
“Low Field”  Ohm’s “Law” holds J  σE or vd  μE
BCS THEORY BCS theory is the first microscopic theory of superconductivity since its discovery in It explains, The interaction of phonons and electrons.
Single-molecule transistors: many-body physics and possible applications Douglas Natelson, Rice University, DMR (a) Transistors are semiconductor.
Electromagnetic Radiation
Insulators, Semiconductors, Metals
Lecture 4 OUTLINE Semiconductor Fundamentals (cont’d)
Coulomb Blockade and Single Electron Transistor
Electromagnetic Radiation
Waves, Light, and the EM Spectrum
Thermal conduction in equilibrium heating heat bath T A
Chapter 5 - Phonons II: Quantum Mechanics of Lattice Vibrations
Waves, Light, and the EM Spectrum
Presentation transcript:

If a 2D metal, also known as a quantum Hall system (QHS), is cooled down to not-too-low temperature, its electrical properties are strongly influenced by lattice vibrations (acoustic phonons). Surprisingly, even though phonons of all different energies below the thermal energy are present, electrons chose to respond to the most energetic phonons they can scatter off. In a magnetic field, electrons’ motion becomes quantized into equally spaced levels and scattering off such phonons is most effective when the phonon energy equals the integer multiple of the inter-level spacing. This leads to oscillations of electrical resistance with magnetic field. We have studied QHS driven by high electrical current in a wide range of temperatures. First, we have demonstrated the possibility to tune and enhance acoustic phonon resonances by dc current. Second, we have observed a prominent peak which emerges when electrons “break the sound barrier”, i.e. when their drift velocity passes through the speed of sound. Finally, unrelated to acoustic phonons, we have demonstrated that dc current can induce a novel state with zero- differential resistance which appears to be an analog of microwave-induced zero resistance states discovered in QHS a few years ago. Nonlinear Transport in Quantum Hall Systems (QHS) Michael A. Zudov, University of Minnesota, DMR Zhang, Zudov, Pfeiffer, West, Physical Review Letters 100, (2008) (a) Differential resistivity vs. dimension- less electric field at magnetic fields from 1 kG to 4 kG in 0.1 kG steps. Some traces (blue) show minima where one normally expects maxima (red). (b) Differential resistance in the magnetic field – dc current plane shows maxima (dark) where conditions for both enhanced phonon and impurity scattering are satisfied (double resonances). (c) At lower temperatures differential resistance might virtually vanish over the finite range of magnetic and electric fields, forming zero- differential resistance state (ZdRS). (a) (b) (c)

Nonlinear Transport in Quantum Hall Systems (QHS) Michael A. Zudov, University of Minnesota, DMR Education: Graduate students: H.-S. Chiang A. Hatke W. Zhang (graduating in 2008). Undergraduate students: Nicholas Eggert ( ) Emily Gras (2007 NSF REU program) Bryan Perfetti ( UROP Program) Students received training in cryogenic, vacuum, and microwave technologies, device nanofabrication, measurement techniques, data acquisition and analysis, programming, and web development. To date, students delivered twelve presentations about their research at conferences, seminars, and Open House events for incoming students. Societal Impact: Understanding electronic devices based on GaAs, one of the most technologically important semiconductors, contributes to advances in device fabrication, making possible applications ranging from fast transistors for cellular phones to lasers for compact disc players. Results were reported at the following conferences: HMF-18, Sao Pedro, Brazil (2008) NanoPeter-2008, St. Petersburg, Russia (2008) QPEQHS, MPIPKS, Dresden, Germany (2008) APS March Meeting, New Orleans (2008) Forschungszentrum, Karlsruhe, Germany (2007) EP2DS-17, Genova, Italy (2007) EPQHS-2, State College, Pennsylvania (2007) APS March Meeting, Denver, Colorado (2007) QHYST06, MPIPKS, Dresden, Germany (2006) More information is available at the group website: