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Continuous Variable Quantum Information: Gaussian States and
Continuous Variable Quantum Information: Gaussian States and

Topological quantum computation
Topological quantum computation

Theory of quantum light emission from a strongly
Theory of quantum light emission from a strongly

... apparent mysteries, perhaps unique to the semiconductor environment. These effects include “off-resonant excitation of the cavity mode” and a “triple peak” during the strong coupling regime. Since these observations are unusual, it has been speculated that they indicate a clear deviation from a sim ...
an introduction to quantum mechanics - TU Dortmund
an introduction to quantum mechanics - TU Dortmund

Is spacetime a quantum error-correcting code?
Is spacetime a quantum error-correcting code?

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An introduction to topological phases of electrons

“Magnus” force - Pacific Institute of Theoretical Physics
“Magnus” force - Pacific Institute of Theoretical Physics

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... A main goal of quantum mechanics is to obtain expectation values for physical observables. If the Wigner function is to be a complete formulation of quantum mechanics, it must also be able to reproduce these expectation values of all functions of x and p. When using Wigner functions the expectation ...
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Regular/irregular phase space structure of HCN/HNC

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Chapter 3: Quantum Computing

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... • Why is N=4 SYM integrable? • What lessons for less supersymmetric SYM and QCD? • 1/N – expansion integrable? • Gluon amlitudes, correlators …integrable? • BFKL from Y-system? ...
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Quantum Information Processing: Algorithms, Technologies and

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Post-quantum Security of the CBC, CFB, OFB, CTR

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Quantum Mechanics

... which are imaginary parts of the respective polyvectors with the -vector component associated with time left out. These constructs are useful because we are going to work in the Hamiltonian formalism where time is singled out. Using them it is straightforward to generalize the standard formalism of ...
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Slides - Agenda

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Implementing Qubits with Superconducting Integrated Circuits Michel H. Devoret and John M. Martinis
Implementing Qubits with Superconducting Integrated Circuits Michel H. Devoret and John M. Martinis

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Viscosity of a nucleonic fluid

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The Liar-paradox in a Quantum Mechanical Perspective

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Three myths about time reversal in quantum theory

Three Myths About Time Reversal in Quantum Theory 1. Introduction
Three Myths About Time Reversal in Quantum Theory 1. Introduction

Commun. Math. Phys. 110, 33-49
Commun. Math. Phys. 110, 33-49

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Quantum group

In mathematics and theoretical physics, the term quantum group denotes various kinds of noncommutative algebra with additional structure. In general, a quantum group is some kind of Hopf algebra. There is no single, all-encompassing definition, but instead a family of broadly similar objects.The term ""quantum group"" first appeared in the theory of quantum integrable systems, which was then formalized by Vladimir Drinfeld and Michio Jimbo as a particular class of Hopf algebra. The same term is also used for other Hopf algebras that deform or are close to classical Lie groups or Lie algebras, such as a `bicrossproduct' class of quantum groups introduced by Shahn Majid a little after the work of Drinfeld and Jimbo.In Drinfeld's approach, quantum groups arise as Hopf algebras depending on an auxiliary parameter q or h, which become universal enveloping algebras of a certain Lie algebra, frequently semisimple or affine, when q = 1 or h = 0. Closely related are certain dual objects, also Hopf algebras and also called quantum groups, deforming the algebra of functions on the corresponding semisimple algebraic group or a compact Lie group.Just as groups often appear as symmetries, quantum groups act on many other mathematical objects and it has become fashionable to introduce the adjective quantum in such cases; for example there are quantum planes and quantum Grassmannians.
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