IRG-3 Electron Spin Coherence of Shallow Donors in Germanium (DMR )

Slides:



Advertisements
Similar presentations
Long-lived spin coherence in silicon with electrical readout
Advertisements

Influence of gases on the formation of atomic gold wires By using a Mechanically Controlled Break Junction (MCBJ) at 4.2 K it is possible to form atomic.
Quantum computing and qubit decoherence
EXAM #3 HAS BEEN MOVED TO MONDAY, NOVEMBER 9 TH Bring a Periodic Table to class this week November 2, 2009.
Image courtesy of Keith Schwab.
Quantum Dots and Spin Based Quantum Computing Matt Dietrich 2/2/2007 University of Washington.
9/22/2004EE 42 fall 2004 lecture 101 Lecture #10 Electrons, Atoms, and Materials Reading: Malvino chapter 2 (semiconductors)
Band Theory & Optical Properties in solids
Lecture 3. Intrinsic Semiconductor When a bond breaks, an electron and a hole are produced: n 0 = p 0 (electron & hole concentration) Also:n 0 p 0 = n.
M. L. W. Thewalt, A. Yang, M. Steger, T. Sekiguchi, K. Saeedi, Dept. of Physics, Simon Fraser University, Burnaby BC, Canada V5A 1S6 T. D. Ladd, E. L.
Frank Bridges, UCSC, DMR Mn La/Ca O Figure 1 Figure 2 Local Structure Studies of La 1-x Ca x MnO 3 : Evidence for Magnetic Dimers We have used.
On Measuring Coherence in Coupled Dangling-Bond Pair Dynamics Zahra Shaterzadeh-Yazdi International Iran Conference on Quantum Information September.
Impurities & Defects, Continued More on Shallow Donors & Acceptors Amusing Answers to Exam Questions Given by Public School Students!
Pressure effect on electrical conductivity of Mott insulator “Ba 2 IrO 4 ” Shimizu lab. ORII Daisuke 1.
This Materials World Network collaborative program brings researchers (Alford and Mayer) from Arizona State University (ASU) and (D. Adams and N. Tile)
ELECTRONIC PROPERTIES OF MATTER - Semi-conductors and the p-n junction -
Temperature and sample dependence of spin echo in SiC Kyle Miller, John Colton, Samuel Carter (Naval Research Lab) Brigham Young University Physics Department.
Large scale quantum computing in silicon with imprecise qubit couplings ArXiv : (2015)
Many solids conduct electricity
Room-Temperature Qubits for Quantum Computing PI: Saritha Nellutla, Department of Chemistry and Biochemistry, Florida State University PI: Gregory S. Boebinger,
Bulk Hybridization Gap and Surface Conduction in the Kondo Insulator SmB 6 Richard L. Greene, University of Maryland College Park, DMR Recently,
المملكة العربية السعودية وزارة التعليم العالي - جامعة أم القرى كلية الهندسة و العمارة الإسلامية قسم الهندسة الكهربائية ELECTRONIC DEVICES K INGDOM.
Single Electron Transistor (SET) CgCg dot VgVg e-e- e-e- gate source drain channel A single electron transistor is similar to a normal transistor (below),
Quenching Spin Decoherence in Diamond through Spin Bath Polarization Gregory S. Boebinger, National High Magnetic Field Laboratory DMR High-Field.
Donor Impurities in Semiconductors as Qubits Cameron Johnson Oct. 26, 2015 Phys 485 Image:
PHYSICAL ELECTRONICS ECX 5239 PRESENTATION 01 PRESENTATION 01 Name : A.T.U.N Senevirathna. Reg, No : Center : Kandy.
INTRINSIC SEMICONDUCTOR  A pure semiconductor.  Its conductivity is low.  It has thermally generated current carries.  Examples of pure or intrinsic.
© Electronics ECE 1312 EECE 1312 Chapter 2 Semiconductor Materials and Diodes.
Semi Conductors Between conductors and insulators are materials, which allow an electric current to flow only under certain circumstances. These are called.
Chemistry Chapter 5 The Periodic Law.
Operational Amplifier
New color centers in diamond for quantum information science
Today’s objectives- Semiconductors and Integrated Circuits
SEMICONDUCTOR FUNDAMENTALS
Impurities & Defects, Continued More on Shallow Donors & Acceptors
N-TYPE AND P-TYPE SEMICONDUCTORS
Introduction to Semiconductor Materials
Introduction to Semiconductors
Modelling & Simulation of Semiconductor Devices
Introduction to Semiconductor Material and Devices.
Teacher Settani Gabriele Montinaro & Giulio Micieli CLIL ELETTRONICA
Elementary Particles (last bit); Start Review for Final
Spin Quantum Number, ms In the 1920s, it was discovered that two electrons in the same orbital do not have exactly the same energy. The “spin” of an electron.
Chemical Bond in Metals and Semiconductors
Electrons: The Bohr Model, Orbitals, and Electron Configuration
|  Introduction to Quantum Computation Bruce Kane
On the collapses and revivals in the Rabi Hamiltonian
General Outcome #1: Investigate technologies that transfer and control electricity.
Introduction to Semiconductor Materials
Nonradiative Quantum Coherences in Semiconductors Hailin Wang, University of Oregon, DMR While storage of classical information is a well- established.
Strong coupling of a superradiant spin ensemble B. C. Rose, A. M
Coupling a Single Electron Spin to a Microwave Cavity
Measurement of Spin Coherence Times in Proton-Irradiated 4H-SiC
SOLIDS AND SEMICONDUCTOR DEVICES - I
SOLID STATE CHMISTRY By: Dr. Aamarpali
Carbon Nanotube Diode Design
Resistance R - _____________________________________
Electron Orbitals Heisenberg 1. The ____________ ______________ principle states that it is impossible to determine simultaneously both the position and.
Choreographing a Whirling Dervish
Majorana Spin Diagnostics
2. Millman & Halikas “ Electronic Devices & Circuits”
The chiral anomaly in a Dirac semimetal
Spin quantum number – ms
Hole Spin Decoherence in Quantum Dots
EE105 Fall 2007Lecture 1, Slide 1 Lecture 1 OUTLINE Basic Semiconductor Physics – Semiconductors – Intrinsic (undoped) silicon – Doping – Carrier concentrations.
Applications in Quantum Computing
Quantum Numbers.
SOLIDS AND SEMICONDUCTOR DEVICES - I
ELECTRICAL PROPERTIES
Subatomic Channeling and Spiraling Electron Beams in Crystals
Presentation transcript:

IRG-3 Electron Spin Coherence of Shallow Donors in Germanium (DMR 01420541) Anthony Sigillito,1 Ryan Jock,1 Alexei Tyryshkin,1 J.W. Beeman,2 E.E. Haller,2,3 Kohei Itoh,4 and Stephen Lyon1 1Princeton University; 2LBNL; 3UC Berkeley; 4Keio University The magnetic moment, or spin, of an electron which is bound to an impurity atom in silicon is exceptionally coherent, an important feature for its use as a quantum bit (qubit) in a quantum computer. However, those electrons are not easily controlled by electric fields. Electron spins in germanium are over 10,000 times more sensitive to an electric field, but it was not known if they would have long coherence. Recently, an international collaboration led by IRG3 researchers have measured electron spin coherence in germanium for the first time.1 The new data show that these electron spins can have coherence times of over 1 ms, and the evidence points to even longer coherence at lower temperatures. These results suggest that germanium is a good material for electron spin qubits. 1. A. Sigillito, et al., Phys. Rev. Lett. 115, 247601 (2015). Fig. 1 Depiction of an arsenic impurity atom (red ball labeled As) in a host crystal of germanium atoms (labeled Ge). The arsenic atom forms chemical bonds with four germanium atoms, but the As atom has one more electron than the Ge atoms. The red arrow indicates the direction of the magnetic moment of this extra electron. Fig. 2 Plots of the time that the spin of the extra electron associated with a phosphorus impurity atom in Ge remains coherent (T2) and does not flip (T1) at different temperatures. At higher temperature the coherence is found to be controlled by an Orbach process, while single phonon processes dominate at lower temperature. At the lowest temperature (0.3 K) the coherence time is over 1 ms.