PeterDonis said:
And even that doesn't exhaust the possibilities: you can pick any integer (positive, negative, or zero) you like, and adopt it as the starting "natural number", and you will satisfy all of the axioms. In other words, there are an infinite number of possible isomorphisms to some "canonical" set of natural numbers (say the ones starting with 1, since those are the ones you say you prefer), each of the form ##x \rightarrow x + a##, with ##a## being any integer.In other words, while it is certainly possible to discover a mapping between a mathematical model and experience in the process of understanding the mathematical model, there is no guarantee that the mapping you discover is the only mapping. So people both using the same mathematical model can still end up making different predictions, if they have not taken steps to ensure that they're both using the same mapping as well. For example, if you use 1-based counting and I use 0-based counting, we're likely to get confused trying to match up our counts if we don't realize the difference and make appropriate adjustments.
Yes, and as I had said in my last post, exactly the same happens in classical mechanics, which can be mapped only up to a rigid motion.
PeterDonis said:
With all that said, I still come back to what I said in my previous post: none of this has anything to do with interpretations of QM, because different interpretations of QM all agree about which mapping between the mathematical model and experiment to use.
No, they don't. Please give me a reference to an online article or well-known textbook that gives this unique ''mapping between the mathematical model and experiment''. And I'll show (like Suppes did) that it says almost nothing about real experiments. Theoretical sources only say something about relations to abstract buzzwords like ''observable'' and ''measure'' about whose precise meaning the interpretations (and the experimental practice) widely differ. There are many thousands of experiments to be covered, the term ''experiment'' in your comment is something very theoretical...
PeterDonis said:
It might be helpful if you would give a concrete example. Perhaps this would qualify as one: the "theory" (for your meaning of that term) is the standard quantum theory of a qubit. Two different possible "mappings" are: interpreting the qubit theory as describing the spin of an electron in a Stern-Gerlach experiment; interpreting the qubit theory as describing the polarization of a photon passing through a beam splitter. Is that the sort of thing you have in mind?
Well this is a meta setting in which the real world is replaced by a theoretical world, in which the qubit has two different interpretations. No, this was not what I had meant.
In your context, consider the qubit first discussed by Weyl 1927 in the context of a Stern-Gerlach-like experiment. [H. Weyl, Quantenmechanik und Gruppentheorie, Z. Phys. 46 (1927), 1-46.] The title of the first part is ''The meaning of the repesentation of physical quantities through Hermitian operators'' (''Bedeutung der Repräsentation von physiksalischen Größen durch Hermitesche Formen''). It discusses among others the paradox that the angular momentum in the three coordinate axes can only take the values ##\pm 1## (in units of ##\hbar/2##) but the angular momentum in other directions, too - which is inconsistent with the algebra. This shows the need for proper interpretation. He then introduces the ensemble interpretation (ensemble = ''Schwarm'') in pure and mixed states, and resolves the paradox in the well-known statistical way. (Thus -
@bhobba,
@atyy - the ensemble interpretation starts at least with Weyl 1927, and not only with Ballentine 1970!)
The map from theory to experiment is stated not as part of the theory but as ''the assumption by Goudsmit and Uhlenbeck, which has proven itself well'' [Goudsmit, S. and Uhlenbeck, G.E., 1926. Die Kopplungsmöglichkeiten der Quantenvektoren I am Atom.
Z. Physik A 35 (1926), 618-625.] - but for electrons, and it was formulated in purely spectroscopic terms. Weyl applies it to a Stern-Gerlach-like experiment (with electrons in place of the original silver atoms).
Why was he allowed to do that? One map from theory to experiment was given through spectroscopy, another map was given through Stern-Gerlach for silver atoms. Fron these, Weyl created by analogy (not by theory) a third map for electrons in the Stern-Gerlach-like experiment. Thus the map changed.
Moreover, there are many more experiments related to angular momentum, and no quantum theory book I know points out how these are connected to the theory.
Nobel prizes are given to new ways of devising useful measurements at unprecedented accuracy, but nobody ever has suggested that each time the theory needs to be amended by mapping its mathematics to these new experimental possibilities. This mapping is described instead in papers published in experimental physics journals!
This is very typical. A theory book gives informally (not as part of the theory, since different expositions of the same theory use different examples) some key experiments in a very simplified description and relates these in an exemplary manner to theory, in order to create suggestive relations between theory and experiment. These are of the same nature as the (according to
@Dale ''highly suggestive'') hints to reality given in a purely mathematical theory to make it intelligible. And they have precisely the same limitations that Dale pointed out:
Dale said:
The mapping to experiment is separate from the mathematical framework itself, even when the names are highly suggestive.
By the same token, the mapping to experiment is separate from the physical theory itself. No theory book gives more than highly suggestive names and pointers to experiments. The connection to real experiments must be made by the experimenter who understands the difference between a real experiment and a symbolic toy demonstration.