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Tailoring Rydberg interactions via F\" orster resonances: state
Tailoring Rydberg interactions via F\" orster resonances: state

Cloaking of Matter Waves
Cloaking of Matter Waves

... Invariant transformation for quantum mechanical systems is proposed. A cloaking of matter wave can be realized at given energy by designing the potential and effective mass of the matter waves in the cloaking region. The general conditions required for such a cloaking are determined and confirmed by ...
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... Originally the weak coupling limit of a finite-size central region interacting with thermal and/or particle baths was first considered [1,2,4–6]. Methods for dealing with the strong coupling limit have been recently developed [7–14]. One can study the NE thermodynamical properties and the entropy pr ...
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Theory and simulation of polar and nonpolar polarizable fluids

... dielectrics. More recently, Stratt and co-workers proposed a nonlinear theory which gives better agreement with simulation than the MSA approximation.22-24 In polar fluids the major contribution to the dielectric constant comes from the permanent dipoles. In this paper we study both kinds of fluids. ...
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... do not know the exact wavefunction Ψ (r1 , .., rA , α1 , .., αN ). We can circumvent this problem by introducing a function which depends on selected variational parameters. This function should capture essential features of the system under consideration. With such a trial wave function we can then ...
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... Gaussian states and Gaussian operations (homodyne detection). Furthermore, we show under which premises concerning entanglement content of the state, noise, inefficient homodyne detectors, our protocol is efficient and applicable with present technology. Our results are reported in [2]. In chapter 5, we ...
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Canonical quantization

In physics, canonical quantization is a procedure for quantizing a classical theory, while attempting to preserve the formal structure, such as symmetries, of the classical theory, to the greatest extent possible.Historically, this was not quite Werner Heisenberg's route to obtaining quantum mechanics, but Paul Dirac introduced it in his 1926 doctoral thesis, the ""method of classical analogy"" for quantization, and detailed it in his classic text. The word canonical arises from the Hamiltonian approach to classical mechanics, in which a system's dynamics is generated via canonical Poisson brackets, a structure which is only partially preserved in canonical quantization.This method was further used in the context of quantum field theory by Paul Dirac, in his construction of quantum electrodynamics. In the field theory context, it is also called second quantization, in contrast to the semi-classical first quantization for single particles.
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