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Reply to criticism of the ‘Orch OR qubit’ – ‘Orchestrated... reduction’ is scientifically justified
Reply to criticism of the ‘Orch OR qubit’ – ‘Orchestrated... reduction’ is scientifically justified

... article [12] in response to Jack Tuszynski (‘JT’), and in also our original review article [2]—though Reimers et al. continually use this terminology. This relates to point (2), a mechanism by which the possible states reduce, or collapse to definite states, the so-called ‘wavefunction collapse’ of ...
Hidden Variables and Nonlocality in Quantum Mechanics
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... Bell [7], and S. Kochen and E. P. Specker [74]. Arguments given by John Stewart Bell1 demonstrate that the prevailing view that these results disprove hidden variables2 is actually a false one. According to Bell, what is shown3 by these theorems is that hidden variables must allow for two important ...
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Holographic Entanglement Entropy - Crete Center for Theoretical
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... (5-1) Basic Outline In principle, we can obtain a metric from a CFT as follows: a CFT state ⇒ Information (~EE) = Minimal Areas ⇒ metric ...
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... equation tend to be proper. 1 Schrodinger equation and Dirac equation are improper Firstly, Schrodinger equation and Dirac equation are not derived by the principle of conservation of energy. As well-known, Schrodinger Equation is actually a basic assumption of quantum mechanics, people can only rel ...
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Classical Mechanics - Mathematical Institute Course Management
Classical Mechanics - Mathematical Institute Course Management

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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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