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Generation of highly entangled photon pairs for continuous variable
Generation of highly entangled photon pairs for continuous variable

... can result in high dimensional entangled states at arbitrary wavelengths if short crystal segments are used. Thus, the technique presented here relies on imposing the condition B ¼ 0 so that the lowest order term in the argument of the N function is quartic in  . Note that for this to be possible ...
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Three Quantum Algorithms to Solve 3-SAT

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... At the present time, most physicists continue to hold a skeptical attitude toward the proposition of a ‘hidden variables’ interpretation of quantum theory, in spite of David Bohm’s successful construction of such a theory and John S. Bell’s strong arguments in favor of the idea. Many are convinced e ...
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Simulations of the angular dependence of the dipole

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... considerable philosophical differences, they almost universally agree on the practical question of what results from a routine quantum physics laboratory measurement (Wheeler, 1983). To describe this, a simple framework to use is the Copenhagen interpretation, the utility of this approach has been v ...
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... two bits for a simulation. Namely, in [29] an extension of the PM square has been introduced, involving 15 different observables in 15 different contexts. The argument goes as follows: consider the 15 observables of the type σµ ⊗ σν where µ, ν ∈ {0, x, y, z} and σ0 = 1 and the case µ = ν = 0 is excl ...
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... a novel hypothesis about the distribution of prime-simplexes that, if solved, may lead to a proof of the Riemann hypothesis. Specifically, if a geometric algorithm predicting the number of prime simplexes within any bound n-simplexes or associated An lattices is discovered, a deep understanding of t ...
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... the basis of the Lindblad quantum master equation [48]. This technique goes beyond the secular approximation and thus can include effects of stronger coupling. However, the approach is still memoryless and leads to time-local evolution equations. Despite the fact that the experimental coherence beat ...
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Renormalization group



In theoretical physics, the renormalization group (RG) refers to a mathematical apparatus that allows systematic investigation of the changes of a physical system as viewed at different distance scales. In particle physics, it reflects the changes in the underlying force laws (codified in a quantum field theory) as the energy scale at which physical processes occur varies, energy/momentum and resolution distance scales being effectively conjugate under the uncertainty principle (cf. Compton wavelength).A change in scale is called a ""scale transformation"". The renormalization group is intimately related to ""scale invariance"" and ""conformal invariance"", symmetries in which a system appears the same at all scales (so-called self-similarity). (However, note that scale transformations are included in conformal transformations, in general: the latter including additional symmetry generators associated with special conformal transformations.)As the scale varies, it is as if one is changing the magnifying power of a notional microscope viewing the system. In so-called renormalizable theories, the system at one scale will generally be seen to consist of self-similar copies of itself when viewed at a smaller scale, with different parameters describing the components of the system. The components, or fundamental variables, may relate to atoms, elementary particles, atomic spins, etc. The parameters of the theory typically describe the interactions of the components. These may be variable ""couplings"" which measure the strength of various forces, or mass parameters themselves. The components themselves may appear to be composed of more of the self-same components as one goes to shorter distances.For example, in quantum electrodynamics (QED), an electron appears to be composed of electrons, positrons (anti-electrons) and photons, as one views it at higher resolution, at very short distances. The electron at such short distances has a slightly different electric charge than does the ""dressed electron"" seen at large distances, and this change, or ""running,"" in the value of the electric charge is determined by the renormalization group equation.
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