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Quantum Techniques for Stochastic Mechanics
Quantum Techniques for Stochastic Mechanics

STABILISED FINITE ELEMENT SOLUTION OF
STABILISED FINITE ELEMENT SOLUTION OF

Cavity Optomechanics in the Quantum Regime
Cavity Optomechanics in the Quantum Regime

Stimulated Scattering of Indirect Excitons in Coupled Quantum Wells
Stimulated Scattering of Indirect Excitons in Coupled Quantum Wells

Excited states from time-dependent density functional theory
Excited states from time-dependent density functional theory

Schaum`s Theory and Problems of Theoretical Mechanics
Schaum`s Theory and Problems of Theoretical Mechanics

Violation of Leggett-Garg inequalities in quantum measurements
Violation of Leggett-Garg inequalities in quantum measurements

... be positive. This requirement results in the LGIs. Specifically, the LGI given by Eq. (1) simply describes the requirement that the probability Pψ (−1, +1) for the measurement outcomes s2 = −1 and s3 = +1 should be positive. Interestingly, fundamental quantum mechanics seems to suggest that these jo ...
Some Useful Formulae for Aerosol Size Distributions and
Some Useful Formulae for Aerosol Size Distributions and

A relevant two qubit Bell inequality inequivalent to the CHSH
A relevant two qubit Bell inequality inequivalent to the CHSH

Quantum Information Processing - wolfgang
Quantum Information Processing - wolfgang

... carried by that state (quantum state collapse). 3. It is extremely difficult to correct errors caused by unwanted interaction with the environment. Nevertheless quantum computational networks can be devised, at least in principle, which are much more efficient, for certain tasks, than classical comp ...
Electroabsorption spectroscopy of effective-mass Al Ga As/GaAs Fibonacci superlattices
Electroabsorption spectroscopy of effective-mass Al Ga As/GaAs Fibonacci superlattices

Conservation of Energy for Unforced Spring
Conservation of Energy for Unforced Spring

Annals of Physics Classical impurities and boundary Majorana zero
Annals of Physics Classical impurities and boundary Majorana zero

Quantum Computing
Quantum Computing

imaging single-electron charging in nanostructures by low
imaging single-electron charging in nanostructures by low

Entropy - Molecular Diversity Preservation International
Entropy - Molecular Diversity Preservation International

... given probability distribution [pi]i, entropy is maximum when all the sent states are orthogonal. I (A : B )  S (%) This inequality is known as the Kholevo (or Holevo) bound, and tells that the average information gain for B in each measurement is bounded by the entropy of the system A. This entrop ...
Leaking Chaotic Systems
Leaking Chaotic Systems

Research Proposal for a Quantum Computer Programming
Research Proposal for a Quantum Computer Programming

... This classical view of the world lasted for hundreds of years until the late nineteenth and early twentieth centuries [12]. It was at this time that the quantum view of the world was uncovered. If the classical view can be described as determinism, then the corresponding description for the quantum ...
Magnetism of 3d Frustrated Magnetic Insulators - Helmholtz
Magnetism of 3d Frustrated Magnetic Insulators - Helmholtz

Quantum Computational Complexity - Cheriton School of Computer
Quantum Computational Complexity - Cheriton School of Computer

Lectures on Random Schrödinger Operators
Lectures on Random Schrödinger Operators

Quantum Information with Optical Continuous Variables - QuIC
Quantum Information with Optical Continuous Variables - QuIC

... In 1905, Einstein took this idea one step further and assumed that the radiation was composed of discrete units of energy, the so called ”quanta”, which allowed him to explain the photo-electric effect [67], which gave him the 1921 Nobel Prize. This revolutionary idea of quantization was applied aga ...
Quantum Correlations in Information Theory
Quantum Correlations in Information Theory

From Molecules to Cooper Pairs: Experiments in the BEC
From Molecules to Cooper Pairs: Experiments in the BEC

Computational Methods for Simulating Quantum Computers
Computational Methods for Simulating Quantum Computers

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Theoretical and experimental justification for the Schrödinger equation

The theoretical and experimental justification for the Schrödinger equation motivates the discovery of the Schrödinger equation, the equation that describes the dynamics of nonrelativistic particles. The motivation uses photons, which are relativistic particles with dynamics determined by Maxwell's equations, as an analogue for all types of particles.This article is at a postgraduate level. For a more general introduction to the topic see Introduction to quantum mechanics.
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