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e ensemble. Let us now proceed to make these ideas more concrete. This interpretation is based on several simple hypotheses: A. Basic hypotheses • Quantum mechanics applies to small subsystems of the universe which come in many copies. Thus, it applies to hydrogen atoms and ammonia molecules, but not t
ger equation from Newtonian mechanics". Phy. Rev.. 150, 1079 (1969): E. Nelson. "Quantum Fluctuations". Princeton Series in Physics. Princeton. [5] L. Smolin. Could quantum mechanics be an approximation to another theory?, quant-ph/0609109. [6] Henrique Comes. Sean Gryb, Tim Koslowski, Einstein gravity as
.com/2073-8994/2/1/230/, J. Kowalski-Glikman, Doubly Special Rel- ativity: facts and prospects, lgr-qc/06030221. [4] H. J. Matschull and M. Welling, Quantum mechanics of a point particle in 2+1 dimensional gravity, Class. Quant. Gray. 15, 2981 (1998) [arXiv:gr-qc/9708054]; For a review see B. J. Schroers
122381; J. Kowalski-Glikman, Observer-independent quanta of mass and length , hep-th/0102098. 18 EFTA_R1_01441409 EFTA02403020 [2] J. Magueijo, L. Smolin, Lorentz invariance with an invariant energy scale, hep-th/0112090, Phys.Rev.Lett. 88 (2002) 190403; Generalized Lorentz invariance with an invarian
0 3.1 Non-locality 10 3.2 Boosts and events 11 3.3 Transverse length contraction and relativity 12 3.4 A classical locality paradox 12 4 Quantum theory of a free relativistic particle 13 4.1 Bases in Hilbert space 13 4.2 Dynamics in momentum space 14 4.3 Dynamics in position space 14
t. B 510 (2001) 255 [arXiv:hep- th/0012238]; J. Kowalski-Glikman, Observer-independent quanta of mass and length , hep- th/0102098. [2] J. Magueijo, L. Smolin, Lorentz invariance with an invariant energy scale, hep-th/0112090, Phys.Rev.Lett. 88 (2002) 190403; Generalized Lorentz invariance with an invarian
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