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2 ( t 2 ′ − t 1 ′ ) 2 − ( x 2 ′ − x 1 ′ ) 2 − ( y 2 ′ − y 1 ′ ) 2 − ( z 2 ′ − z 1 ′ ) 2 (all events 1, 2) . 4-tuple b of numbers are added to events a1 and a2. Such transformations are referred to as spacetime translations and should not handled additional here. Finding the solution to the simpler problem is just a matter of look-up in the theory of classical teams that preserve bilinear types of various signature. The choice notation defined on the right is referred to because the relativistic ...
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