PPT-Quantum State of the Union

Why a Retreat Why a Center Transforming Caltech Quantum Science Prehistoric Feynman Thorne Premillennial Preskill 1983 Vahala 1986 Kimble 1989 Yeh 1989 Eisenstein 1996. 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. 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.. and the monogamy of entanglement. Aram . Harrow (MIT). Brown SUMS. March 9, 2013. Quantum mechanics. QM has also explained:. the stability of atoms. the photoelectric effect. e. verything else we’ve looked at. 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:. 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 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. Dung Nguyen. Chicago 19. th. January. Content. Motivation . Quantum bit (qubit) vs Classical bit (bit). Quantum Computation . Quantum Communication. Conclusion. Motivation. The end of Moore’s law scaling in silicon (because of quantum effects of particle at scale smaller than 7nm).. 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 . 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. ..