vanhees71 said:
Well, of course, to measure the position of a particle you need a different device than to meausure its momentum. This is not specific to QT but also the case within classical physics. Indeed there's no problem with this, and it's in no way mystical at all.
The difference is that in classical mechanics you an in principle have several measurement devices at once, measuring all things at once without distorting the system. Ie. you can have a "collection of observers" asking all kinds of questions at once, and then simlpy joing the answers.
This is not possible in quantum mehanics, and its Bohrs point with complementarity.
In this case the measurent is "trivial" or marginalized to a practical matters in classical matter. In quantum mechanics, the choice of measurements distorts the system, in a way that that dependes on what you choose to measure. This is the "subjectivity".
But there is no point in disagreeing on the word. I think we roughly agree at the basic level. I just wanted to express that even though i may not share Demystifiers view, i still follow the objections and point of subjectivity (give or take the choice of words).
vanhees71 said:
I've also never understood Bohr's "classical measurement device". According to QT everything is quantum, including macroscopic systems making up measurement devices. The classical behavior of the relevant macroscopic observables (which are coarse-grained by averaging many microscopic degrees of freedom over microscopically large, macroscopically small space-time regions) is emergent.
You can not in Borhs view properly speak of what is quantum without a classical reference. Surely, you can view the apparatous + system as another "new quantum system" BUT, then you need ANOTHER classical backdrop. To think you can repeat this until you end up with a complete wavefunction of the universe is IMO a fallacy that makes no sense. I think this is Bohrs point. But if we get into the details here, atl east i will raise questions that i think is beyond the scope of the original Einstein Bohr dispute. Bohrs point is I think the most acccurate one if you consider quantum theory as it stands. Even field theory needs a backdrop. The detectors must be attached in a classical world.
To generalized things beyond that, then we are at BTSM discussions.
There is IMO also a connection between when the Newtonian schema works (as per Smolin) AND Bohrs requirement for aclassical backdrop. Without the classical backdrop, which also severs the purposes of information sink, there is no rigid reference for the Newtonian schema - and we need a new understanding of physical law.
/Fredrik
