PPT-Quantum One: Lecture 13

1 2 More about Linear Operators 3 In the last lecture we stated and explored the consequences of the 2 nd postulate of the general formulation of quantum mechanics which associates observables with . with a . Scala. Embedded . Language. Xiao Liu and . John . Kubiatowicz. Computer Science Division. University of California, Berkeley. Email: {. xliu. , . kubitron. }@eecs.berkeley.edu. Why Quantum Computers?. Chapter 12. E-mail: . benzene4president@gmail.com. Web-site: http://clas.sa.ucsb.edu/staff/terri/. Quantum – . ch 12. 1. A photon has a frequency (v) of 5.45 x 10. 8. MHz. a. Calculate the photons wavelength (λ) in nm. Modern Physics. 5/10/11 . Spring 2011. Ben Miller, Alexander . DeCarli. , Kevin Shaw. What is it?. How do particles become Entangled?. Parametric Down Conversion. A laser (usually ultraviolet for its high frequency) sends a photon through a nonlinear crystal such as Beta Barium Borate. Quantum Hamiltonian Complexity. Aram Harrow (MIT). Simons Institute. 16 Jan 2014. Entanglement. Original motivation for quantum computing. [Feynman ‘82]. Nature isn't classical, dammit, and if you want to make a simulation of Nature, you'd better make it quantum mechanical, and by golly it's a wonderful problem, because it doesn't look so easy.. OverviewIntroduction •Methods of Intermixing•Quantum Wells•Ion Implantation Induced InterdiffusionLasers, PhotodetectorsImpurity Free InterdiffusionIntegrated Waveguide-Quantum Dots Dieter Jaksch. Outline. Lecture 1: Introduction. What defines a quantum simulator? Quantum simulator criteria. Strongly correlated quantum systems.. Lecture 2: Optical lattices. Bose-Einstein condensation, adiabatic loading of an optical lattice. and . Ultra-Efficient Solar Cells . 2008. “for the Layman”. Disclaimer. The information contained in this document is provided by Phoenix Alliance Corp. through its research sources and is obtained from sources that Phoenix Alliance Corp. believes to be reliable or are otherwise expressions of third party opinion. Whilst Phoenix Alliance Corp. has made reasonable efforts to ensure the accuracy, completeness and appropriateness of such information, any reliance on such information is entirely at the risk of the party using it, and it will not rely on such contents in substitution for making proper and appropriate enquiries from the relevant third parties. . “. Kaleidoscope . of Exotic Quantum Phases in a Frustrated XY Model. ,”. Christopher N. Varney, Kai Sun, Victor . Galitski. , and Marcos . Rigol. , . Phys. Rev. . Lett. ., . 107. , 077201 (2011) (also chosen for Editor’s suggestion and . MAS 725. Hartmut. . Klauck. NTU. 12.3.2012. Topics . today. Superdense. . coding. Distinguishing quantum states. Bell . inequalities. Superdense Coding. Alice . has two . b. its of classical information she wants to send to Bob. Fang Song. IQC, University of Waterloo. -- “Quantum-Friendly” Reductions. 2. How do . quantum . attacks change classical cryptography?. Crypto-systems based on the hardness of factoring and discrete-log are . McsQPT. ). Joint work with: . S. . Rahimi-Keshari. , A. T. . Rezakhani. , T. C. Ralph. Masoud. Ghalaii. Nov. 2013. 1. Basic concepts—Phase space, Wigner . function, . HD, … . Harmonic oscillator. n, l, m, and s. Used to . describe. an . electron. in an . atom. Probable location. n. Principal Quantum Number. Represents . main. energy level of . electron. Maximum. # . o. f . electrons. in an . Khalid Muhammad. 1. History of Quantum Computing. Bits and Qubits. Problems with the Quantum Machine. Who Introduced the Idea?. Khalid Muhammad. 1. Introduction to Quantum Computing. Soviet scientist Yuri . Part 1. Outline. Introduction. Problems of classical physics. Black-body Radiation. experimental observations. Wien’s displacement law. Stefan – Boltzmann law. Rayleigh - Jeans. Wien’s radiation law.