quantum gravity
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6 matching pages
1: 32.16 Physical Applications
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►For the Ising model see Barouch et al. (1973), Wu et al. (1976), and McCoy et al. (1977).
►For applications in 2D quantum gravity and related aspects of the enumerative topology see Di Francesco et al. (1995).
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2: Bibliography F
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Discrete Painlevé equations and their appearance in quantum gravity.
Comm. Math. Phys. 142 (2), pp. 313–344.
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3: 18.39 Applications in the Physical Sciences
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4: Bibliography C
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Quasinormal modes of the extremal BTZ black hole.
Classical Quantum Gravity 21 (12), pp. 2801–2809.
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5: Bibliography D
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The constrained quantum mechanical harmonic oscillator.
Proc. Cambridge Philos. Soc. 62, pp. 277–286.
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Quantum Fields and Strings: A Course for Mathematicians. Vol. 1, 2.
American Mathematical Society, Providence, RI.
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D gravity and random matrices.
Phys. Rep. 254 (1-2), pp. 1–133.
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6: 22.19 Physical Applications
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►With the same initial conditions, if the sign of gravity is reversed then the new period is ; see Whittaker (1964, §44).
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►plays a prototypal role in classical mechanics (Lawden (1989, §5.2)), quantum mechanics (Schulman (1981, Chapter 29)), and quantum field theory (Pokorski (1987, p. 203), Parisi (1988, §14.6)).
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►Such solutions include standing or stationary waves, periodic cnoidal waves, and single and multi-solitons occurring in diverse physical situations such as water waves, optical pulses, quantum fluids, and electrical impulses (Hasegawa (1989), Carr et al. (2000), Kivshar and Luther-Davies (1998), and Boyd (1998, Appendix D2.2)).
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