neither the state of the actual system, nor the system itself, corresponds to anything in the math.
Your first source says, specifically, that the result is not tested against observations (which is false, e.g. double slit) and the second says that the relation between the mathematics and the physical reality is an open question.
You, however, appear to be arguing not that the relationship cannot be determined. You are arguing that the relationship somehow can be determined as
unequal - the mathematics
definitely do not match up with the physical system. My opinion is that you're not only wrong, but fundamentally cannot support the argument you're trying to make - because the physical process actually going on is
completely ineffable and opaque apart from via the mathematics formalisms. You cannot compare the two and say they don't match, because
you don't have anything to compare the formalism to.
If you read the description above carefully, you'll notice exactly what you asked for (once again): the "system" and the "states" are entirely prepared by macroscopic devices (which allow some actual quantum system to run), but the quantum processes which result from the set-up are never related directly to the mathematical formalisms which are then called the "system".
But how do you know? What do you know of the quantum processes that are
literally unobservable? (We know by pure experiment that observing them changes the processes significantly, without having to touch quantum theory itself.)
The initial state is specified macroscopically and is described by parameters set in advance in a deterministic manner at odds with what quantum theory holds is true of quantum dynamics via some formalism...
I'm not sure how setting up the experiment in a "deterministic" way is at odds with quantum theory, at least in a way that isn't trivially fixable by an application of conditional probability.
Also, are you looking for classical-type measurements or not?
...every time you refer to a source on "quantum systems", "measurements", and "states", these are not described by actual physical states, measurements, or systems, but by the theorized states which are always abstracted from the actual quantum systems and which are always specified macroscopically and deterministically so that there can be a "measurement" and a "system" and some "states", but nobody knows how the mathematics correspond to actual quantum systems, quantum states, or anything else...
You apparently do, since you assert that the theory
does not match the actual quantum system right at the beginning of the paragraph.
But this means that any "measurement" cannot be a measurement of the state of the system.
Quantum theory tells us a measurement is a thing you do to a system, which 1) produces a value, which is the value you end up measuring, and 2) disturbs the system in a non-reversible way. It is very similar to what we'd think of a measurement of the system, apart from the irreversible modification part.
It's preparing your "system" as if it were someone with a bow and arrow, ...announce that the distribution of the debris is where the aarrow landed.
As you keep telling idav,
it's not really like that, since the arrow keeps landing in one piece and in one place,
despite the fact that not only is your arrow imperfectly manufactured in a way you can't measure with absolute precision, it seems to do wibbly-wobbly things in the air that are impossible to formulate with any sort of accepted aerodynamics knowledge.
If they are counterfactually definite, then we can't use quantum mechanics.
Wavefunctions aren't counterfactually definite - they do not produce definite predictions, only probabilistic distributions.
Attempts to formulate a coherent framework with purely quantum rules taking into account the environment have however failed to provide a consistent picture of quantum mechanics and the measurement process."
I am not surprised. AFAIK, a measurement with a quantum doodad is, as is logical, not a measurement in the sense of an non-unitary operator application, which is what happens if you use a classical device to do the measuring.
If one doesn't treat the environment as classical, then obviously you run into an issue because now you've got more quantum objects than the SI standards committee had prefixes for.
Of course, it is generally agreed that, as a result of the decoherence predicted, under any normally realistic conditions, by the QM formalism itself, it is no longer possible to see the effects of interference between the two or more ‘branches’ of the superposition. However, the quantum formalism is exactly the same at the microscopic and the macroscopic level; if, therefore, a given interpretation is excluded in the former case, it cannot become permitted in the latter!
There seems to be a gap in this logic. I don't understand how they conclude that the quantum formalism is required to change if one is to say that decoherence means that the two states of the cat don't interact.
If you figure that out, let physicists know. You'll get a nobel prize at least.
Everett already did that part for me - the quantum state is the thing being described by the formalism.
What formal system? The system is a model of physics. If it's "pure mathematics", we wouldn't have physicists. We'd just have mathematicians.
The physicists are there to construct the model out of experiments. Mathematics can derive theorem results without reference to experiment, e.g. Bell's theorem.
Certainly if you don't actually work that into your equations. But that's what's done.
Then I shall just have to learn enough to do it myself.
Sure, if you haven't any clue how both are actually understood and how both relate to the QCC/quantum-to-classical transition issues.
The vanishing
h technique is used to show, purely mathematically, that QM implies classical results in the domain of classical physics, e.g. large lengths, small energies produce negligible superpositions. If this didn't work,
we'd have a major problem, since it'd mean that QM disagrees fundamentally with a theory validated by experiment. However, even though this works, it says nothing about QM's validity
outside the domain of classical physics.
What we seem to be arguing about is why, despite quantum mechanics wibbliness, we experience a sensible, Newtonian reality, which is an empirical result that doesn't connect to any mathematical relationship between classic and quantum mech. More on this later.
And should you take away Einstein's nobel prize?
I thought Einstein's Nobel was for the photoelectric effect.
Or disregard Schroedinger? Or how about the PhD's of all the authors, from those writing papers (such as "Quantum Correlations in Biomolecules" from 22nd Solvay conference on Chemistry), or perhaps from the authors of studies/reviews such as these:
Or any number of sources I've already mentioned (which continually gets me links to wiki articles or even less) on the utter inadequacy of this "vanishing h".
As mentioned, the measurement problem is not related to vanishing h. In fact, using the vanishing h technique
implies the measurement problem, because if you accept quantum theory as a good descriptor, to the point where you want to derive classic results from it, then you... accept quantum theory's indeterminism as a good descriptor of reality, and so you need to explain why reality we experience appears classical.
It doesn't. But it does fundamentally conflict with your view. Because in it our measurements our meaningless. Macroscopic reality is the constant splitting of universes into parallels. So if you think that reality is "computed" by the universe, then you are in absolute disagreement with Everett, whose theory literally involves constant, total, and ever-present superpositions represented only in parallel universes, but never observed, measured, or represented by any physical systems in one universe.
I agree with Everett entirely, because of my choice of what, precisely, reality is computing: the universal wavefunction. As Everett dictates,
every possibility is equally real, and the entire universe forms a deterministically-evolving tree of superpositions and entangled particles. There's nothing problematic about computing that in principle.
Also, my interpretation has an ace in te hole that I believe Copenhagen does not share. If Everett and myself are wrong in saying that reality is quantum and our Newtonian view of reality is the result of sufficiently complicated entanglement, then answer me this question:
How do quantum computers work when there is too little information content in the universe to store their wavefunction? (e.g. a 500-qubit quantum computer requires 2^500 bits of information to store its wavefunction; the information capacity of the universe is ~2^160 bits.)