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... C =C -parity is a useful quantum number for particles which are their own antiparticles and are eigenstates of Cˆ , eg  0 ,  , . Can also be extended into G-parity (later). Ca ,Ca are arbitary phase factors with no physical significance. Cˆ changes the sign of all "internal" quantum numbers: cha ...
A New Quantum Behaved Particle Swarm Optimization
A New Quantum Behaved Particle Swarm Optimization

... This paper presents a variant of Quantum PSO called Q-QPSO, incorporating the concept of recombination operator. The proposed Q-QPSO is tested on three standard unconstrained benchmark test problems and the results are compared with some of the existing QPSO (containing mutation operator) and standa ...
A Global Equilibrium as the Foundation of Quantum
A Global Equilibrium as the Foundation of Quantum

A New Quantum Behaved Particle Swarm Optimization
A New Quantum Behaved Particle Swarm Optimization

... it on 10 benchmark problems (unconstrained) given in Table 1. All the test problems are highly multimodal and scalable in nature and are considered to be starting point for checking the credibility of any optimization algorithm. There is not much literature available in which QPSO is used extensive ...
Quantum Random Walk via Classical Random Walk With Internal
Quantum Random Walk via Classical Random Walk With Internal

... random walk, the behavior of a (classical) particle moving on a line according to some probabilistic rule is studied. In the simplest model, a particle will move, at every discrete time step, one unit to the left or to the right with probabilities p and 1 − p, respectively, independent of its past ...
Many-body physics gravitational Lens
Many-body physics gravitational Lens

... effective as the velocity of a pair is increased. This behavior is now called the “hot wind effect,” because in the rest frame of the quark pair the wind of the passing QGP is seen to weaken their interaction. Based on this observation, we predicted that the production rate of bound states formed fr ...
Bose-Einstein condensation of excitons and cold atoms OECS13
Bose-Einstein condensation of excitons and cold atoms OECS13

ppt - Harvard Condensed Matter Theory group
ppt - Harvard Condensed Matter Theory group

W3: Reversible Quantum Computing
W3: Reversible Quantum Computing

here - IFT
here - IFT

Quantum Mechanical Path Integrals with Wiener Measures for all
Quantum Mechanical Path Integrals with Wiener Measures for all

Fault-Tolerant Quantum Computation
Fault-Tolerant Quantum Computation

Information measures, entanglement and quantum evolution Claudia Zander
Information measures, entanglement and quantum evolution Claudia Zander

Non-classical computing - Mathematical and Computer Sciences
Non-classical computing - Mathematical and Computer Sciences

... can conceptualise systems capable of computing with real number quantities (for example a quantum computer is modelled with qubits which are parameterised by unconstrained real values and evolve continuously in time) but, even if physical systems do in fact function “objectively” in this way (this i ...
Statistics lecture (Powerpoint)
Statistics lecture (Powerpoint)

... • Quote means and uncertainties to a level of precision consistent with the uncertainty, e.g: 3.77±0.08 kg, not 3.77547574568±0.08564846795768 kg. • Quote units on all numerical values ...
Quantum telescopes
Quantum telescopes

God, Belief and Explanation
God, Belief and Explanation

Quantum Numbers and Rules
Quantum Numbers and Rules

PDF
PDF

... Lie algebroid, or globally in terms of a special Lie (or Lie–Weinstein) symmetry groupoid representations that can also take into account the spin exchange interactions between the Jahn–Teller centers exhibiting such quantum dynamic effects. Unlike the simple symmetries expressed by group representa ...
Quantum Criticality: competing ground states in low
Quantum Criticality: competing ground states in low

Angle Matrix Elements
Angle Matrix Elements

... where r̂ denotes the set of coordinates θ, φ giving the direction of the unit vector r̂ = r/r is not well known. The version given here is from Jackson, Classical Electrodynamics, 2nd Ed., Eq. (3.70). The whole point of this formula is to separate the variables of particle 1 from the variables of pa ...
Time Evolution of States for Open Quantum
Time Evolution of States for Open Quantum

The non-equilibrium Green`s function method
The non-equilibrium Green`s function method

... In quantum transport, the treatment of boundary conditions requires significantly more care than in classical physics due to the nonlocality of quantum mechanics.19-22 A common problem is to define Ohmic leads. In the context of NEGF, we may define leads as Ohmic if the current is controlled by the ...
Part 1 - Capri Spring School
Part 1 - Capri Spring School

Learning about order from noise Quantum noise studies of
Learning about order from noise Quantum noise studies of

... Correlation function measurements after TOF expansion. Extra Bragg peaks appear in the second order correlation function in the AF phase. ...
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Quantum entanglement

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