PPT-Moments Coherent-State Quantum Process Tomography (

McsQPT Joint work with S RahimiKeshari A T Rezakhani T C Ralph Masoud Ghalaii Nov 2013 1 Basic conceptsPhase space Wigner function HD Harmonic oscillator. Superluminescent. Emitter. Ahmed Musse, Deborah . Varnell. , Mei Chai . Zheng. , . Nyan. . Aung. , . Germano. . Penello. , and . Claire . Gmachl. Department of Electrical Engineering, Princeton . University. What’s the problem? . Quantum limits on noise in phase-preserving linear amplifiers. The whole story. Completely positive maps and physical . ancilla. states. Immaculate linear amplifiers. The bad news. 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.. John . Stachel. Frontiers of Fundamental Physics 14. Epistemology and Philosophy. Marseille, 17 July 2014 . Do Quanta Need a New Logic?. Three Aspects of . a. Logic. Syntax. : . A formalism, or set of symbols and rules for well-formed formulas using these symbols. Collection of two-state quantum systems (. qubits. ). Operations which manipulate isolated . qubits. or pairs of . qubits. Initialise. . qubit. to . single state. Detect . qubit. state. Large scale device:. Lecture . 9. Optical Coherence Tomography. David J. Brady. Duke University. Lecture 9. Optical coherence tomography. www.disp.duke.edu/~dbrady/courses/holography. Outline. Huang paper. Tomography. OCT and light-in-flight holography. and the monogamy of entanglement. Aram . Harrow. MIT (UCL until Jan 2015). Quantum mechanics. QM has also explained:. the stability of atoms. the photoelectric effect. e. verything else we’ve looked at. Byron Smith. December 11, 2013. What is Quantum State Tomography?. What is Bayesian Statistics?. Conditional Probabilities. Bayes. ’ Rule. Frequentist. vs. Bayesian. Example: . Schrodinger’s Cat. 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.. Aram Harrow. . based on joint work with . Fernando G.S.L. Brandão. (ETHZ->Imperial). PCP theorem. Classical k-CSPs:. Given constraints . C={C. i. }. , choose an assignment . σ. mapping . n. variables to an alphabet . Monroe. University of Maryland. Quantum Simulations. with Atoms. Aarhus. Amherst. Basel. Berkeley. Bonn. Citadel. Clemson. Denison. Duke. Erlangen. ETH-Zurich. Freiburg. Georgia . Tech. Griffith . Hannover. Daniel Reitzner. Research Center for Quantum Information, Slovak Academy of Sciences. 1st . eduQUTE. school on quantum technologies. Bratislava 19-22/02/2018. Welcome notes. Do not hesitate to ask questions anytime during the talk if something will be unclear!. University of Maryland. Department of Physics. National Institute of. Standards and Technology. Hardware. “. There's Plenty of Room . at . the Bottom. ” (1959. ) . “. When we get to the very, very small world – say circuits of . Tel Aviv University. Nir Bitansky. Omri Shmueli. Zero-Knowledge Protocols . [Goldwasser, . Micali. , . Rackoff. 85].  . .. .. .. Accept/Reject.  .  .  . This work:. ZK against quantum attacks. ..