We are improving our search experience. To check which content you have full access to, or for advanced search, go back to the old search.

Search

Please fill in this field.

Search Results

Showing 1-20 of 10,000 results
  1. Introduction

    The state of a physical system is the mathematical description of our knowledge of it, and provides information on its future and past. A state...
    Matteo G.A. Paris, Jaroslav Řeháček in Quantum State Estimation
    Chapter
  2. 2 Quantum Tomographic Methods

    The state of a physical system is the mathematical object that provides a complete information on the system. The knowledge of the state is...
    Giacomo Mauro D’Ariano, Matteo G.A. Paris, Massimiliano F. Sacchi in Quantum State Estimation
    Chapter
  3. 9 Quantum Operations on Qubitsand Their Characterization

    Information encoded in quantum system has to obey rules of quantum physics which impose strict bounds on state estimation and on possible...
    Francesco De Martini, Marco Ricci, Fabio Sciarrino in Quantum State Estimation
    Chapter
  4. 8 Characterization of Quantum Devices

    Using quantum tomography and a single entangled state it is possible to characterize completely a quantum device, a channel, or a measuring...
    Giacomo Mauro D’Ariano, Paoloplacido Lo Presti in Quantum State Estimation
    Chapter
  5. Method of Invariant Grids

    The method of invariant grids is developed for a grid-based computation of invariant manifolds.
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  6. Mathematical Notation and Some Terminology

    – The operator L from space W to space E: L : W → E
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  7. References

    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  8. Invariance Equation in Differential Form

    Definition of invariance in terms of motions and trajectories assumes, at least, existence and uniqueness theorems for solutions of the original...
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  9. Entropy, Quasiequilibrium, and Projectors Field

    Projection operators Py contribute both to the invariance equation (3.2), and to the film extension of the dynamics (4.5). Limiting results, exact...
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  10. Geometry of Irreversibility: The Film of Nonequilibrium States

    A geometrical framework of nonequilibrium thermodynamics is developed in this chapter. The notion of macroscopically definable ensembles is...
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  11. Film Extension of the Dynamics: Slowness as Stability

    One of the difficulties in the problem of reducing the description is caused by the fact that there exists no commonly accepted formal definition of...
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  12. Accuracy Estimation and Post-Processing in Invariant Manifolds Construction

    The post-processing algorithms are developed for the accuracy control and enhancement of approximate invariant manifold.
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  13. Method of Natural Projector

    P. and T. Ehrenfest introdused in 1911 a model of dynamics with a coarse-graining of the original conservative system in order to introduce...
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  14. Relaxation Methods

    The “large step**” relaxation method for solution of the invariance equation is developed.
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  15. Slow Invariant Manifolds for Open Systems

    Suppose that the slow invariant manifold is found for a dissipative system. What have we constructed it for? First of all, for solving the Cauchy...
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  16. Quasi-Chemical Representation

    In Chap. 5 we have used the second law of thermodynamics, the existence of the entropy, in order to equip the problem of constructing the slow...
    Alexander N. Gorban, Ilya V. Karlin in Invariant Manifolds for Physical and Chemical Kinetics
    Chapter
  17. 6 Quantum Tomography from Incomplete Data via MaxEnt Principle

    We show how the maximum entropy (MaxEnt) principle can be efficiently used for a reconstruction of states of quantum systems from incomplete...
    Vladimír Bužek in Quantum State Estimation
    Chapter
  18. 11 Discrimination of Quantum States

    The problem of discriminating among given nonorthogonal quantum states is underlying many of the schemes that have been suggested for quantum...
    János A. Bergou, Ulrike Herzog, Mark Hillery in Quantum State Estimation
    Chapter
  19. 12 Quantum States: Discrimination and Classical Information Transmission.A Review of Experimental Progress

    The purpose of this chapter is to review the experimental achievements made to date in two closely related areas of quantum information science....
    Anthony Chefles in Quantum State Estimation
    Chapter
  20. 3 Maximum-Likelihood Methodsin Quantum Mechanics

    Maximum Likelihood estimation is a versatile tool covering wide range of applications, but its benefits are apparent particularly in the quantum...
    Zdeněk Hradil, Jaroslav Řeháček, ... Miroslav Ježek in Quantum State Estimation
    Chapter
Did you find what you were looking for? Share feedback.