This is a very interesting essay, Neil. I'll need to wake up and review your proposal more carefully before really commenting on it, but from a first reading, your thought experiment strikes me as very 'Einsteinian', reminiscent of the arguments he used to challenge Bohr's conception of quantum mechanics. I mean that as a compliment: Einstein may have been wrong, but his thinking nevertheless was often clearer than that of his opponents.
However, one thing I'm not sure I got is the asymmetry of knowledge between the 'preparer' and the 'measurer' of a quantum system. I mean, most preparation procedures are essentially measurements: you prepare a spin up electron by letting it traverse an appropriately aligned Stern-Gerlach apparatus and blocking the path of the spin-down component, i.e. effectively you measure, and just keep those systems whose measurement result produces the outcome you want to keep. After that measurement, the preparer has 'perfect knowledge' about the electron, at least in the 'up/down' basis.
Now consider the situation of a measurer, who perhaps might choose to measure in some orthogonal basis. He will obtain evenly distributed statistics, and after measurement, will have perfect knowledge about the state of each electron in that basis, but no knowledge about the prior state of the electron in the 'up/down' basis. But does this mean that he has access to 'less' information than the preparer has?
I think to a certain extent, two different things are being compared here: knowledge in the 'up/down' and in an orthogonal, say 'left/right'-basis. After preparation, the preparer has zero knowledge about the electron in the 'left/right'-basis, just as the measurer; after the measurement, his knowledge is perfect in that basis, but all knowledge about the 'up/down'-state is destroyed.
So at various points, both the preparer and the measurer possess perfect knowledge about the electron, but their knowledge is (as Bohr would say) complementary: it can't coexist. The asymmetry, it seems to me, comes about only if you describe things in one basis (that of the preparer). That, I think, would as a description be better suited to the case in which both measure in the same basis: but of course, then the measurer can obtain all the information the preparer has.
But anyway, I think your larger point still stands: there is indeed more information in the quantum state than can be extracted classically. The simplest demonstration of this is that it takes a huge (in principle, infinite) amount of information to perfectly describe the state of even a single qubit, since it is given by a point on the Bloch sphere, of which there are continuously many; yet one can always extract a maximum of one bit of information through measurement. In general, the extractable amount of information is of course given by Holevo's bound. Nevertheless, you can sometimes do neat tricks like dense coding, i.e. transferring two bits of information through the sending of a single qubit.
There's another way to see that quantum information exceeds classically available information, which is through considering the amount of information that can be communicated: if I have access to a qubit's worth of information, I couldn't share that with you, since I can't clone. The best I can do is to just measure, and share the result. In fact, this is one way to characterize the 'truly quantum' part of information: it's the part you can't share.
Anyway, I'll go and have a look at your essay again; hope you'll do well.