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  1. Antiparticles from special Relativity with ortho-chronous and antichronous Lorentz transformations.Erasmo Recami & Waldyr A. Rodrigues - 1982 - Foundations of Physics 12 (7):709-718.
    Special Relativity can be based on the whole proper group of both ortho- and antichronous Lorentz transformations, and a clear physical meaning can be given also to antichronous (i.e., nonorthochronous) Lorentz transformations. From the active point of view, the latter requires existence, for any particle, of its antiparticle within a purely relativistic, classical context. From the passive point of view, they give rise to frames “dual” to the ordinary ones, whose properties—here briefly discussed—are linked with the fact that in relativity (...)
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  • The theory of relativity.Christian Møller - 1952 - Oxford,: Clarendon Press.
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  • A vector product formulation of special relativity and electromagnetism.Charles P. Poole, Horacio A. Farach & Yakir Aharonov - 1980 - Foundations of Physics 10 (7-8):531-553.
    The vector product method developed in previous articles for space rotations and Lorentz transformations is extended to the cases of four-vectors, anti-symmetric tensors, and their transformations in Minkowski space. The electromagnetic fields are expressed in “six-vector” form using the notationH +iE, and this vector form is shown to be relativistically invariant. The wave equations of electromagnetism are derived using these vector products. The following three equations are deduced, which summarize electrodynamics in a compact form: (1) Maxwell's four equations expressed as (...)
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