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A1993LX38200001
A1993LX38200001

... at Johns Hopkins. Years later, as a visiting ...
Quantum Spacetime without Observers: Ontological
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... states that in certain classical limits, quantum theory should reproduce the predictions of classical theory with vanishing errors. In particular, for those objects which are known to be in excellent agreement with classical mechanics — chairs, planets, etc. — quantum effects should be negligible. I ...
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... Macroscopic systems exhibit three important properties (features) distinguishing them from microscopic systems: 1. In macroscopic systems occur irreversible processes leading to equilibrium states in which the properties of the system do not depend on time (and there are no mass flows). 2. The equil ...
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Davies Maps - Fernando Brandao

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... distinguished. Quite often the coordinates of space and the position variables of a point particle are denoted by the same symbols x, y, z (e.g. when one writes ψ(x, y, z, t) for the wave function of a particle). To avoid this confusion we shall denote the dynamical position variables of a particle ...
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... describe the physical degrees of freedom also at the very smallest distances. The first attempt of quantizing gravity relied on canonical quantization, with the spatial metric components and their conjugate momenta as the canonical variables, and the Wheeler-DeWitt equation governing the dynamics [3 ...
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COVARIANT HAMILTONIAN GENERAL RELATIVITY
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... variations in the 1930’s. In section 2, I briefly illustrate the main lines of this formulation using the example of a scalar field, and I discuss its relation with the relativistic notions of state and observable considered in Ref. 1 I then apply these ideas to general relativity (GR) in Section 3. ...
if on the Internet, press  on your browser to
if on the Internet, press on your browser to

... in the modern theoretical physics of quantum gravity, topological field theory, and conformal field theory. The spin-off from his twistor theory and his early attempts at quantum geometry is significant. Penrose's original spin networks for SU(2) have been extended to any Lie group G even to categor ...
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Quantum gravitational contributions to quantum electrodynamics

... The potential importance of the original calculation 13 stimulated a number of further investigations that cast doubt on its findings. It was shown 15 that a different choice of gauge condition led to the absence of any quantum gravity correction to the Yang-Mills β-function. Because of the possible ...
< 1 ... 21 22 23 24 25 26 27 28 29 ... 38 >

Canonical quantum gravity

In physics, canonical quantum gravity is an attempt to quantize the canonical formulation of general relativity (or canonical gravity). It is a Hamiltonian formulation of Einstein's general theory of relativity. The basic theory was outlined by Bryce DeWitt in a seminal 1967 paper, and based on earlier work by Peter G. Bergmann using the so-called canonical quantization techniques for constrained Hamiltonian systems invented by Paul Dirac. Dirac's approach allows the quantization of systems that include gauge symmetries using Hamiltonian techniques in a fixed gauge choice. Newer approaches based in part on the work of DeWitt and Dirac include the Hartle–Hawking state, Regge calculus, the Wheeler–DeWitt equation and loop quantum gravity.
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