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Quantum mechanics in more than one
Quantum mechanics in more than one

Quantum Dots - Paula Schales Art
Quantum Dots - Paula Schales Art

... J. Lee et al Adv. Materials, 12, 1102 (2000) ...
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Bethe-Salpeter Equation with Spin
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... Some physicists try to derive probabilities of actual outcomes directly from field theory, without a Hamiltonian or potential. Is the idea of a potential only an approximation suitable for some energy scales? – I would ask: Are there not still some roles for mass, kinetic and ...
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Quantum Control in Cold Atom Systems
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Exercises for Quantum Field Theory (TVI/TMP)
Exercises for Quantum Field Theory (TVI/TMP)

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PPT - Fernando Brandao

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... Gauge symmetry is not a symmetry. It is a fake, a redundancy introduced by hand to help us keep track of massless particles in quantum field theory. All physical predictions must be gauge-independent. In an ordinary quantum field theory without gravity, in flat spacetime, there two types of physical ...
Quantum Teleportation
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Physics 351: Advanced Classical Mechanics Spring 2013
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PPT - LSU Physics & Astronomy

... loss in order to maximize the extraction of the available phase information in an interferometer. Our approach optimizes over the entire available input Hilbert space with no constraints, other than fixed total initial photon number. ...
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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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