Is there any non-trivial sense in which the spacetime symmetries in the SM gauge QFT are made local?
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This is not in general a reasonable thing to expect to be able to do. In SR, these coordinate transformations will only work locally. The coordinates can only be extended to a distance x∼c2/a away from the observer's world-line, where a is the acceleration of the observer. At greater distances, the coordinate transformation isn't one-to-one. In GR, coordinate systems do not describe observers
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An attempt is made to develop a (speculative) picture on ``quantum symmetry" which links space-time symmetries in an inexorable way with internalsymmetries.
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