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Fredrik said:The idea that I used as the starting point is that a theory must be able to assign probabilities to statements of the form"If you use the measuring device [itex]\delta[/itex] on the object [itex]\pi[/itex], the result will be in the set [itex]E[/itex]".
So your approach is to let "measuring device" be an abstract term. But what is supposed to be the interpretation? Suppose we have as a simple case a universe consisting of nothing but a single spin-1/2 particle fixed in place (so the only degrees of freedom are from spin). I assume that the "observables" in this case are associated with the set of 2x2 hermitian matrices. Which means, in terms of Pauli spin matrices [itex]\sigma_i[/itex], that they are of the form:
[itex]A + B_i \sigma_i[/itex], where [itex]A, B_x, B_y, B_z[/itex] are 4 real numbers. So for this toy theory, each such matrix is a measuring device?
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