cGh physics

cGh physics refers to the historical attempts in physics to unify relativity, gravitation and quantum mechanics, in particular following the ideas of Matvei Petrovich Bronstein and George Gamow.[1][2] The letters are the standard symbols for the speed of light (c), the gravitational constant (G), and Planck's constant (h).

A depiction of the cGh cube
Diagram showing where quantum gravity sits in the a near-cube hierarchy of physics theories. Note that electromagnetism and quantum field theory in curved spacetime are added in as an extra and distinct items.

If one considers these three universal constants as the basis for a 3-D coordinate system and envisions a cube, then this pedagogic construction provides a framework, which is referred to as the cGh cube, or physics cube, or cube of theoretical physics (CTP).[3] This cube can used for organizing major subjects within physics as occupying each of the eight corners.[4][5] The eight corners of the cGh physics cube are:

Other cGh subjects include Planck units, Hawking radiation and black-hole thermodynamics.

While there are several other physical constants, these three are given special consideration, because they can be used to define all Planck units and thus all physical quantities.[6] The three constants are therefore used sometimes as a framework for philosophical study and as one of pedagogical patterns.[7]

Overview

Before Ole Rømer made the first successful estimate of the speed of light in 1676, it was not known whether the speed of light (c) was infinite or not. Because of the tremendously large value of c (i.e. 299,792,458 metres per second in vacuum) compared to the speeds of things in our daily experience, the propagation of light seems to us to be instantaneous. Hence, the ratio 1/c was hidden from our view making relativistic mechanics irrelevant. At speeds comparable to the speed of light (c), special relativity takes the finitude of the speed of light into consideration by the aid of Lorentz transformation. A non-relativistic theory is recovered from a relativistic theory when the limit 1/c is set to zero.

The gravitational constant (G) is irrelevant for a system where gravitational forces are negligible. For example, the special theory of relativity is the special case of general relativity in the limit G → 0.

Similarly, in the theories where the effects of quantum mechanics are irrelevant, the value of Planck constant (h) can be neglected. For example, setting h → 0 in the commutation relation of quantum mechanics, the uncertainty in the simultaneous measurement of two conjugate variables tends to zero, approximating quantum mechanics with classical mechanics.

References
  1. Kragh, Helge (2009). "Relativistic Quantum Mechanics". In Greenberger, Daniel; Hentschel, Klaus; Weinert, Friedel (eds.). Compendium of Quantum Physics. Berlin, Heidelberg: Springer. pp. 632–637. doi:10.1007/978-3-540-70626-7_184. ISBN 978-3-540-70622-9. Retrieved 2022-03-23.
  2. Kragh, Helge (1995). "Review of Matvei Petrovich Bronstein and Soviet Theoretical Physics in the Thirties". Isis. 86 (3): 520. doi:10.1086/357307. ISSN 0021-1753. JSTOR 235090.
  3. Padmanabhan, Thanu (2015). "The Grand Cube of Theoretical Physics". Sleeping Beauties in Theoretical Physics. Springer. pp. 1–8. ISBN 978-3319134420.
  4. Gorelik, Gennady E. (1992). "First Steps of Quantum Gravity and the Planck Values". Studies in the History of General Relativity. Birkhäuser. pp. 364–379. ISBN 978-0-8176-3479-7. Archived from the original on 2019-04-25. Retrieved 2009-05-07.
  5. Wainwright, C.J. "The Physics Cube". Archived from the original on 6 March 2012.
  6. Duff, Michael; Lev B. Okun; Gabriele Veneziano (2002). "Trialogue on the number of fundamental constants". Journal of High Energy Physics. 2002 (3): 023. arXiv:physics/0110060. Bibcode:2002JHEP...03..023D. doi:10.1088/1126-6708/2002/03/023. S2CID 15806354.
  7. Okun, Lev (1991-01-01). "The fundamental constants of physics". Soviet Physics Uspekhi. 34 (9): 818–826. Bibcode:1991SvPhU..34..818O. doi:10.1070/PU1991v034n09ABEH002475.
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