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  1. Spontaneous para-Lorentzian conserved-vector and nonconserved-axial weak currents.J. G. Vargas - 1982 - Foundations of Physics 12 (8):765-779.
    The energy-momentum relationship is obtained in para-Lorentzian dynamics. It is shown that the well-known correspondence rule for the operators energy and momentum holds in any inertial system if it is assumed to hold in the preferred reference frame. The new Dirac equation is obtained. Some qualitative features of the new theory are given; one of then is the spontaneous appearance of conserved-vector and nonconserved-axial weak currents. Finally one evaluates the convenience of further developments of the present theory in view of (...)
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  • Nonrelativistic para-Lorentzian mechanics.J. G. Vargas - 1981 - Foundations of Physics 11 (3-4):235-278.
    After reviewing the foundations of special relativity and the room left for rival theories, a set of nonrelativistic para-Lorentzian transformations is derived uniquely, based on (a) a weaker first principle, (b) the requirement that the transformations sought do not give rise to the clock “paradox” (in a refined version), and (c) the compliance of the transformations with the classical experiments of Michelson-Morley, Kennedy-Thorndike, and Ives-Stilwell. The corresponding dynamics is developed. Most of the experimental support of special relativity is reconsidered in (...)
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  • Mach, Einstein, and the rise of modern science.Elie Zahar - 1977 - British Journal for the Philosophy of Science 28 (3):195-213.
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