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Special relativity and quantum mechanics

Englewood Cliffs, N.J.,: Prentice-Hall (1968)

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  1. From the Group SL(2, C) to Gyrogroups and Gyrovector Spaces and Hyperbolic Geometry.Jingling Chen & Abraham A. Ungar - 2001 - Foundations of Physics 31 (11):1611-1639.
    We show that the algebra of the group SL(2, C) naturally leads to the notion of gyrogroups and gyrovector spaces for dealing with the Lorentz group and its underlying hyperbolic geometry. The superiority of the use of the gyrogroup formalism over the use of the SL(2, C) formalism for dealing with the Lorentz group in some cases is indicated by (i) the validity of gyrogroups and gyrovector spaces in higher dimensions, by (ii) the analogies that they share with groups and (...)
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  • Algebraic field descriptions in three-dimensional Euclidean space.Nikos Salingaros & Yehiel Ilamed - 1984 - Foundations of Physics 14 (8):777-797.
    In this paper, we use the differential forms of three-dimensional Euclidean space to realize a Clifford algebra which is isomorphic to the algebra of the Pauli matrices or the complex quaternions. This is an associative vector-antisymmetric tensor algebra with division: We provide the algebraic inverse of an eight-component spinor field which is the sum of a scalar + vector + pseudovector + pseudoscalar. A surface of singularities is defined naturally by the inverse of an eight-component spinor and corresponds to a (...)
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  • Extension of trigonometric and hyperbolic functions to vectorial arguments and its application to the representation of rotations and Lorentz transformations.H. Yamasaki - 1983 - Foundations of Physics 13 (11):1139-1154.
    The use of the axial vector representing a three-dimensional rotation makes the rotation representation much more compact by extending the trigonometric functions to vectorial arguments. Similarly, the pure Lorentz transformations are compactly treated by generalizing a scalar rapidity to a vector quantity in spatial three-dimensional cases and extending hyperbolic functions to vectorial arguments. A calculation of the Wigner rotation simplified by using the extended functions illustrates the fact that the rapidity vector space obeys hyperbolic geometry. New representations bring a Lorentz-invariant (...)
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