Kainui said:
For instance, in the double slit experiment I'm told that observation is what causes the wave function to collapse.
There is a problem to start with.
If even wavefunction collapse occurs is interpretation dependent eg it doesn't happen in MWI. And in interpretations where is does occur if it actually means anything is debatable. Throw a dice and before trowing it its state is represented by 1/6th attached to each face. After the throw its state has collapsed to a 1 (ie a dead cert) on some face. Nothing but this conceptual thing called probabilities has changed.
I have posted this in another thread, but I find this the best way to understand exactly what the formalism of QM is saying - not what it means - that is another issue - but what its saying. However before trying to figure out what it means, its wise to understand what it says
My view, purely on the basis of the formalism, without entering into the quagmire of these interpretational issues, is its simply what's required to allow us to predict the probabilities of outcomes of observations, similar to what probabilities themselves are. Indeed the differences between some interpretations is simply a variant of the different ways you can interpret probabilities ie frequentest or Bayesian, but I won't go into that right now.
I will base the following on the two axioms in Ballentine - QM - A Modern development, which is a very well respected textbook on QM - many people like myself think of it as THE textbook - its that good. Its a very interesting fact that QM really rests on just two axioms. There is a bit more to it, but they are more or less along the lines of reasonableness assumptions such as the probability of outcomes should not dependent on coordinate systems ie symmetry.
Imagine we have a system and some observational apparatus that has n possible outcomes associated with values yi. This immediately suggests a vector and to bring this out I will write it as Ʃ yi |bi>. Now we have a problem - the |bi> are freely chosen - they are simply man made things that follow from a theorem on vector spaces - fundamental physics can not depend on that. To get around it QM replaces the |bi> by |bi><bi| to give the operator Ʃ yi |bi><bi| - which is basis independent. In this way observations are associated with Hermitian operators. This is the first axiom in Ballentine, and heuristically why its reasonable.
Next we have this wonderful theorem, Gleason's theorem, which, basically, follows from the above axiom:
http://kof.physto.se/theses/helena-master.pdf
This is the second axioms in Ballentine's treatment.
This means a state is simply a mathematical requirement to allow us to calculate expected values in QM. It may or may not be real - there is no way to tell. Its very similar to the role probabilities play in probability theory. In fact in QM you can also calculate probabilities. Most people would say probabilities don't exist in a real sense and why I personally don't think the state is real - but that's just my view - as far as we can tell today its an open question.
Basically QM is a theory about the probabilities of outcomes of observation, if we were to observe it. The sole purpose of a state is, when combined with an observable, is to allow us to predict the probabilities of the outcomes of observations. And exactly like probabilities its very existence is to change to some outcome when you conduct the experiment, observation or whatever.
Again, this has nothing to do with what it MEANS. Different interpretations have different takes on that. But purely from the formalism that's what it's about.
Thanks
Bill