Microscopic relativity: The basic theory

Authors
Citation
R. Lieu, Microscopic relativity: The basic theory, FOUND PHYS, 31(8), 2001, pp. 1233-1250
Citations number
7
Categorie Soggetti
Physics
Journal title
FOUNDATIONS OF PHYSICS
ISSN journal
00159018 → ACNP
Volume
31
Issue
8
Year of publication
2001
Pages
1233 - 1250
Database
ISI
SICI code
0015-9018(200108)31:8<1233:MRTBT>2.0.ZU;2-Z
Abstract
In effort to investigate how quantum physics might modify Einstein's Theory of Relativity tit speeds v --> c, the relationship between space-time coor dinates of different reference frames is revisited by introducing only one new parameter x(o), a fundamental constant for the quantization of space. T he starting point is three criteria: (a) real space-time data are condition ed by standard quantum effects on measurements, (b) since currently used ap paratus are only capable of probing the aggregate behavior of these quanta the relevant model is one which maximizes the Entropy subject to certain de fining constraints; and (c) the constraints simply involve fixed ensemble a verages in the case of an inertial frame, or boundary conditions on running averages in the case of an accelerated frame. In this context it is found that both the Lorentz transformation and a simple scheme for the quantizati on of space-time which resembles identically, Planck's photon picture of ra diation are a direct consequence of the Principle of Relativity. Non-inerti al behavior corresponds to local Entropy maxima, obtainable by solution of a diffusion equation which gives gradually varying ensemble averages across space-time, as demonstrated by the example of a profile which connects a c entral region of highly agitated quanta with an asymptotic ambient environm ent-the outcome is the Schwarzschild metric of General Relativity. Apart fr om the above, a new feature emerges from the theory: the space-time data of an observer, when referred to the frame of his moving partner, are subject to extra quantum fluctuations which increase indefinitely in severity as v --> c, with the Lorentz transformation providing only the mean data values . Thus for fast moving bodies like cosmic rays or matter at the horizon of a black hole, physical processes which affect them may not always be percei ved by its to occur at the expected length or time scales.