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tom.stoer
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Find, thanks (but I am curious to understand how you can agree to my realist or even platonist position)vanhees71 said:I couldn't agree more with this part of your posting. Indeed QT doesn't contradict this "simple philosophical position" at all. Only the notion of what a state is. In classical physics it's described by a point in phase space, in QT by the statistical operator of the system. The main difference between the classical description and quantum description is that in the classical case by the complete knowledge of the state one knows the values of all possible observables of this system (i.e., the values of all observables are always determined), while in QT only a well-defined class of observables take determined values, when any (pure or mixed) state of the system is prepared.
This is just to increase circulation. I don't give a damn.vanhees71 said:... let alone even in this modern form as "many-worlds interpretation" with the world branching into many parallel universes at any observation ...
That is an interesting question, yes.vanhees71 said:... which also brings in the famous funny question by Bell, whether the observation of something by an amoeba is enough to cause a collapse (or in the MW interpretation the branching of the world) or whether you need some "more intelligent being" like a dog, monkey or human (who knows, how intelligent an amoeba maybe might be, but we just don't know it ;-)).
This is a possible consequence, but not necessarily a logical one. It simply denies the idea to let science provide realistic (ontic) explanations. Of course yours is one possible philosophical position, but there are others. They may not be yours, but they do not go away.vanhees71 said:I think the logical consequence is the minimal interpretation, according to which QT is a formalism to describe probabilistically what we observe objectively in this real world, which you describe above. Indeed, as the name says, the quantum state describes the state of the system, and it's not a state vector but the statistical operator (or equivalently in the case of pure states, which are in general quite rare and must be carefully prepared in the lab, rays in Hilbert space).
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