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Relativity of quantum superpositions
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In modern physics only relative quantities are considered to have physical significance. For example, position assigned to a system depends on the choice of coordinates, and only relative distances between different systems have physical relevance. On the other hand, in quantum theory the scenario where one system, A, is localised around certain position while another system B is in a spatial superposition is considered to be physically different from the scenario where A is in a superposition, while B is localised. Different physical effects are anticipated in the two scenarios especially when the two systems have widely different masses. Here we show that for any superposed amplitudes that are related by a symmetry transformation, the above scenarios are physically equivalent: probabilities for any measurement are the same whether we assign the superposition state to system A or to system B. More generally, linearity of quantum theory guarantees that if a theory is invariant under some symmetry transformations it is necessarily also invariant under their arbitrary `superpositions'. Thus the notion of a superposition turns out to be relative to the choice of coordinates, once it is realised that relations between coordinates do not need to be classical.
Forward citations
Cited by 2 Pith papers
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Quantum clocks and the temporal localisability of events in the presence of gravitating quantum systems
An event is time-delocalised from the perspective of other gravitationally interacting clocks but always sharply localised from the perspective of the clock that triggers it.
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Gravitational entanglement witness through Einstein ring image
A mass source in quantum superposition produces multiple Einstein rings in a quantized Newtonian gravity model but a single ring in the Schrodinger-Newton model, with a new 'which-path' indicator vanishing in the latter.
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