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  1. Tachyon kinematics and causality: A systematic thorough analysis of the tachyon causal paradoxes. [REVIEW]Erasmo Recami - 1987 - Foundations of Physics 17 (3):239-296.
    The chronological order of the events along a spacelike path is not invariant under Lorentz transformations, as is well known. This led to an early conviction that tachyons would give rise to causal anomalies. A relativistic version of the Stückelberg-Feynman “switching procedure” (SWP) has been invoked as the suitable tool to eliminate those anomalies. The application of the SWP does eliminate the motions backwards in time, but interchanges the roles ofsource anddetector. This fact triggered the proposal of a host of (...)
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  • The introduction of Superluminal Lorentz transformations: A revisitation. [REVIEW]G. D. Maccarrone & Erasmo Recami - 1984 - Foundations of Physics 14 (5):367-407.
    We revisit the introduction of the Superluminal Lorentz transformations which carry from “bradyonic” inertial frames to “tachyonic” inertial frames, i.e., which transform time-like objects into space-like objects, andvice versa. It has long been known that special relativity can be extended to Superluminal observers only by increasing the number of dimensions of the space-time or—which is in a sense equivalent—by releasing the reality condition (i.e., introducing also imaginary quantities). In the past we always adopted the latter procedure. Here we show the (...)
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  • On some frequent but controversial statements concerning the Einstein-Podolsky-Rosen correlations.O. Costa de Beauregard - 1985 - Foundations of Physics 15 (8):871-887.
    Quite often the compatibility of the EPR correlations with the relativity theory has been questioned; it has been stated that “the first in time of two correlated measurements instantaneously collapses the other subsystem”; it has been suggested that a causal asymmetry is built into the Feynman propagator. However, the EPR transition amplitude, as derived from the S matrix, is Lorentz andCPT invariant; the correlation formula is symmetric in the two measurements irrespective of their time ordering, so that the link of (...)
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