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Under such extreme conditions, space-time cannot be treated as a classical continuum and must be given a quantum interpretation.
The consistent histories, also known as decoherent histories, approach to quantum interpretation is broadly compatible with standard quantum mechanics as found in textbooks.
These are known as acoustic lattice vibrations or, in the quantum interpretation, as acoustic phonons.
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This is the basic reason why the first measurement problem M1 is an enormous difficulty for quantum interpretations in which the only possible time dependence for a closed quantum system is that given by Schrödinger's equation.
For a further discussion of the quanta interpretation see the subsection on inequivalent representations below.
Note that for Fraser's negative conclusion about the tenability of the particle (or quanta) interpretation for QFT there is no need to assume localizability.
For Bain, the occurrence of UIRs without a particle (or quanta) interpretation for intervening times, i.e. close to scattering experiments, is irrelevant because the data that are collected from those experiments always refer to systems with negligible interactions.
Fraser (2008) rates this as an unsuccessful "last ditch" attempt to save a quanta interpretation of QFT because it is ad hoc and can't even show that at least something similar to the free field total number operator exists for finite times, i.e. between the asymptotically free states.
Quantum chemical interpretation of such reduction sequence is provided.
All phenomena, including gravitational interactions, have an underlying quantum-mechanical interpretation.
An important and interesting topic in quantum mechanics is interpretation of the uncertainty relation, which was first expounded by Heisenberg [1].
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