Results 211 to 220 of about 66,624 (250)

Random Transitions of a Binary Star in the Canonical Ensemble. [PDF]

Entropy (Basel)
Chavanis PH.
europepmc   +1 more source

Landauer Principle and the Second Law in a Relativistic Communication Scenario. [PDF]

Entropy (Basel)
Alvim YJ, Céleri LC.
europepmc   +1 more source

Unique conformational dynamics and protein recognition of A-to-I hyper-edited dsRNA. [PDF]

Nucleic Acids Res
Müller-Hermes C, Piomponi V, Hilber S, Asami S, Kreutz C, Bussi G, Sattler M.   +6 more
europepmc   +1 more source

On the relation of canonical and covariant formulations of Loop Quantum Gravity

, 2015
Antonia Zipfel
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Transmembrane association of DDR1 and DDR2 mediated by Leucine zipper motifs. [PDF]

Magn Reson Lett
Huang F, Li Y, Zhang P, Li J, Xie C, Wang J, Cai T.   +6 more
europepmc   +1 more source

Nonperturbative solutions for canonical quantum gravity

Nonperturbative solutions for canonical quantum gravity
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Functional integrals and canonical quantum gravity

Physical Review D, 1992
The functional-integral sum-over-histories formulation of quantum gravity in the canonical Arnowitt-Deser-Misner formalism is examined. Reduced phase-space quantization (RPSQ) is contrasted with Dirac quantization (DQ). While it does not appear that RPSQ is even defined for gravity, there do exist minisuperspace models in which different ...
, Guven, , Ryan
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Time and the interpretation of canonical quantum gravity

Physical Review D, 1989
The unsatisfactory status of the interpretation of the wave function of the Universe in canonical quantum gravity is reviewed. The ``naive interpretation'' obtained by straightforwardly applying the standard interpretive rules to the canonical quantization of general relativity is manifestly unacceptable; the ``WKB interpretation'' has only a limited ...
, Unruh, , Wald
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Canonical approach to quantum gravity

Classical and Quantum Gravity, 1987
Summary: Dirac's canonical programme for the quantization of gravity is discussed. The order of operators in the `kinetic' part of the generator of normal deformations, \(\hat H_{\perp}\), is chosen to give the Laplace-Beltrami form. This follows from the requirement of invariance of the quantum theory under arbitrary contact transformations of the ...
Christodoulakis, Theodosios, Zanelli, Jorge   +1 more
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