The Bizarre Quantum Nature of Light. Nergis Mavalvala Massachusetts Institute of Technology August 2005. Einstein’s Annus Mirabilis. 1905 Photoelectric effect Special theory of relativity 1916 General theory of relativity 1922 Nobel prize for the photoelectric effect 1935

ByA Layered Software Architecture for Quantum Computing Design Tools. Krysta M. Svore , Alfred V. Aho Columbia University Andrew W. Cross, Isaac Chuang Massachusetts Institute of Technology Igor L. Markov University of Michigan January 2006. Outline. Introduction Background

ByPrinciple of equal a priori probabilities: An isolated system, with N,V,E, has equal probability to be in any of the W (N,V, E ) quantum states or Each and every one of the W (N,V, E ) quantum states is represented with equally probability. Principle of equal a priori probability.

ByDiscrete Phase-Space Structure and MUB Tomography. Andrei B. Klimov J.L. Romero, G.Bjork, L.L. Sanchez-Soto. Palermo 07. Motivation. Standard N - qubit state tomography: Number of measurement sets: Indirect measurement of DM elements accumulation of errors

ByMultipartite Entanglement Measures from Matrix and Tensor Product States. Ching -Yu Huang Feng -Li Lin Department of Physics, National Taiwan Normal University arXiv:0911.4670. Outline. • Quantum Phase Transition • Entanglement measure • Matrix/Tensor Product States

ByElectron Configuration. Quantum States and Orbitals. Quantum state = a specific combination of values of variables such as energy and position that is allowed by quantum theory. We group electrons into different quantum states to describe their electron arrangement.

ByJosephson qubits. P. Bertet. SPEC, CEA Saclay (France ), Quantronics group. Outline. Lecture 1: Basics of superconducting qubits. Lecture 2: Qubit readout and circuit quantum electrodynamics. Lecture 3: 2- qubit gates and quantum processor architectures.

ByPH300 Modern Physics SP11. “ I will never believe that god plays dice with the universe. ” - Albert Einstein. 3/8 Day 15: Questions? Repeated spin measurements Probability. Thursday: Entanglement Quantum Physics & Reality Quantum Cryptography. Last Week:

ByQuantum-Cloning. Valerio Scarani - Chapter Three. Context. 1982 Wooters and Zurek Nature 1982 Dieks Asher Peres http:// arxiv.org/PS_cache/quant-ph/pdf/0205/0205076v1.pdf No classical error correction! ( but Q Error Corr. possible, Shor )

ByPhysical Fluctuomatics 13th Quantum-mechanical extensions of probabilistic information processing. Kazuyuki Tanaka Graduate School of Information Sciences, Tohoku University kazu@smapip.is.tohoku.ac.jp http://www.smapip.is.tohoku.ac.jp/~kazu/. Contents. Introduction

ByWritten Reports for Measurements Lab. Logistics: when and where Content: what to talk about Technique: Organization, presentation. Logistics. When: See schedule What you will turn in: One report per group Turn in answers to questions

BySchool of Physics and Astronomy FACULTY OF MATHEMATICAL AND PHYSICAL SCIENCES. “Classical entanglement” and cat states. Jacob Dunningham. Paraty, August 2007. Overview. The consequences of entanglement: The emergence of classicality from the quantum world Number and phase of BEC

ByThe Center for Quantum Information. Engineering entanglement: How and how much?. Alfred U’ren Pablo Londero Konrad Banaszek Sascha Wallentowitz Matt Anderson Christophe Dorrer Ian A. Walmsley. Approaches. • Manipulating quantum fields.

ByQuantum-optics experiments in Olomouc. Palacký University & Institute of Physics of AS CR. Jan Soubusta, Martin Hendrych , Jan Pe řina, Jr., Ondřej Haderka. Antonín Černoch, Miroslav Gavenda, Eva Kachlíková, Lucie Bartůšková. Radim Filip, Jaromír Fiurášek, Miloslav Dušek.

ByEntangling Atoms with Optical Frequency Combs.

ByQuantum Teleportation and Bit Commitment. Chi-Yee Cheung Chung Yuan Christian University June 9, 2009. What are teleportation and bit commitment?

ByQuantum Computers, Algorithms and Chaos , Varenna 5-15 July 2005. Quantum computation with solid state devices - “Theoretical aspects of superconducting qubits”. Rosario Fazio. Scuola Normale Superiore - Pisa. “DiVincenzo list”. Two-state system Preparation of the state

ByQuantum Information, Communication and Computing. Jan Kříž. Department of physics, University of Hradec Králové Doppler Institute for mathematical physics and applied mathematics. Quantum Information, Communication and Computing.

ByChapter 13 Classical & Quantum Statistics. 13.1 Boltzmann Statistics It deals distinguishable, non-interacting particles. There are two constrains N J = N N J · ε J = U where N J is the number of particles with single-particle energy ε J.

ByExperimental Issues in Quantum Measurement. Lectures: Tuesday, 10-11, Kleiner Hörsaal. Aephraim Steinberg. (auf Englisch, es tut mir leid). Why does one thing happen and not another? When is a quantum measurement? Does a measurement necessarily disturb the system, and how?

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