Abstract:Two broad scenarios for extended linear Lorentz transformations (ELTs) are modeled in Section 2 for mixing subluminal and superluminal sectors resulting in standard or deformed energy-momentum dispersions. The first scenario is elucidated in the context of four diverse realizations of a continuous function (V), with 0 ≤ (V) ≤ 1 and (0) = () = 1, which is fitted in the ELT. What goes in the making of the ELT in this scenario is not the boost speed V, as ascertained by two inertial observers in uniform relative … Show more
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