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Transcript of Speech by Professor Stephen Hawking
Transcript of Speech by Professor Stephen Hawking

Stationary entanglement and discord for dissipating qubits by local
Stationary entanglement and discord for dissipating qubits by local

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... molecule are quantized, each with its own characteristic energy. Motions of the molecule as a whole— rotations and vibrations—have the lowest energies, in the 1–100 millielectron volt regime (1 meV = 10-3 eV). An electron volt, abbreviated eV, is the energy an electron gains falling through a potent ...
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The Semiotic Flora of Elementary Particles

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Full Text PDF - Science and Education Publishing

... preferential direction; the precession is characterized by the precession phase, angle of deflection, and precession frequency; b) spin correlations may take place between the spins of pairs of virtual particles. The 2nd concept. In the physical vacuum there may exist quantum harmonic oscillators po ...
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... • The relation H = T + U = E is valid ONLY under the conditions of the derivation (!): – The eqtns of transformation connecting rectangular & generalized coords must be independent of time  T is a homogeneous, quadratic function of qj. – Then potential energy U must be independent of the generalize ...
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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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