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      Relativity in space-times with short-distance structure governed by an observer-independent (Planckian) length scale

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          Abstract

          I show that it is possible to formulate the Relativity postulates in a way that does not lead to inconsistencies in the case of space-times whose short-distance structure is governed by an observer-independent length scale. The consistency of these postulates proves incorrect the expectation that modifications of the rules of kinematics involving the Planck length would necessarily require the introduction of a preferred class of inertial observers. In particular, it is possible for every inertial observer to agree on physical laws supporting deformed dispersion relations of the type \(E^2- c^2 p^2- c^4 m^2 + f(E,p,m;L_p)=0\), at least for certain types of \(f\).

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          Severe Limits on Variations of the Speed of Light with Frequency

          Explosive astrophysical events at high red shift can be used to place severe limits on the fractional variation in the speed of light (\(\Delta c/c\)), the photon mass (\(m_{\gamma}\)), and the energy scale of quantum gravity (\(E_{QG}\)). I find \(\Delta c/c < 6.3 \times 10^{-21}\) based on the simultaneous arrival of a flare in GRB 930229 with a rise time of \(220 \pm 30 \mu s\) for photons of 30 keV and 200 keV. The limit on \(m_{\gamma}\) is \(4.2 \times 10^{-44} g\) for GRB 980703 from radio to gamma ray observations. The limit on \(E_{QG}\) is \(8.3 \times 10^{16}\) GeV for GRB 930131 from 30 keV to 80 MeV photons.
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            One Hundred Years of Quantum Physics

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              Author and article information

              Journal
              14 December 2000
              2000-12-26
              Article
              10.1142/S0218271802001330
              gr-qc/0012051
              9cc070fe-a646-47c8-b27b-ab33d5a8ae14
              History
              Custom metadata
              Int.J.Mod.Phys. D11 (2002) 35-60
              Same formulas and results as in 1st version, but a change of notation is introduced in order to clarify that the studied illustrative example is consistent with the R.P. for both choices of the overall sign. 1 ref added and 2 refs upgraded. Some rewording of the text in Sec5, and addition of an analogy with background fields in ordinary electromagnetism which I use to illustrate difference between space-times with an observer-independent Lp, and space-times in which Lp is introduced without modifications of Special Relativity
              gr-qc

              General relativity & Quantum cosmology
              General relativity & Quantum cosmology

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