Lord Jestocost
Mario Rossi said:So the observer effect does not make a quantum system 100% deterministic, right?
Let me answer with a section of the paper “Decoherence, the measurement problem, and Interpretations of quantum mechanics“ by Maximillian Schlosshauer (https://arxiv.org/abs/quant-ph/0312059)
II. THE MEASUREMENT PROBLEM
One of the most revolutionary elements introduced into physical theory by quantum mechanics is the superposition principle, mathematically founded in the linearity of the Hilbert state space. If |1i and |2i are two states, then quantum mechanics tells us that any linear combination α|1i+β|2i also corresponds to a possible state. Whereas such superpositions of states have been experimentally extensively verified for microscopic systems (for instance, through the observation of interference effects), the application of the formalism to macroscopic systems appears to lead immediately to severe clashes with our experience of the everyday world. A book has never been ever observed to be in a state of being both “here” and “there” (i.e., to be in a superposition of macroscopically distinguishable positions), nor does a Schroedinger cat that is a superposition of being alive and dead bear much resemblance to reality as we perceive it. The problem is, then, how to reconcile the vastness of the Hilbert space of possible states with the observation of a comparatively few “classical” macrosopic states, defined by having a small number of determinate and robust properties such as position and momentum. Why does the world appear classical to us, in spite of its supposed underlying quantum nature, which would, in principle, allow for arbitrary superpositions?
And now, with respect to decoherence and the measurement problem:
Joos and Zeh remarked on decoherence as a source of spatial localization: "Of course no unitary treatment of the time dependence can explain why only one of these dynamically independent components is experienced." (E. Joos and H. D. Zeh, Zeitschrift Phys. B 59, 223–243; 1985).
Joos states in another article: “Does decoherence solve the measurement problem? Clearly not. What decoherence tells us is that certain objects appear classical when observed. But what is an observation? At some stage we still have to apply the usual probability rules of quantum theory.” (Joos, E. (1999) ‘Elements of Environmental Decoherence’, in P. Blanchard, D. Giulini, E. Joos, C. Kiefer and I.-O. Stamatescu (eds.), Decoherence: Theoretical, Experimental, and Conceptual Problems (New York: Springer), pp. 1-17.)
Or, as Nikolaus von Stillfried remarks: “In his Essay 'Lifting the fog from the north' (Nature 453, 39; 2008), Maximilian Schlosshauer describes how the process of decoherence can explain the famous double-slit experiment. An electron interacting with innumerable quanta in the photographic plate (and its environment) becomes entangled with all of them — and the resulting collective wavefunction is so narrow that it appears particle-like.
But the question remains as to why the wavefunction narrows in precisely the location where it does, or - as Schlosshauer puts it - "Why is a single spot here and not there?"
The author's somewhat 'foggy' answer is suggestive of a version of Everett's 'many worlds' idea (see Nature 448, 15–17; 2007), in which all possible branches of the wavefunction continue to exist autonomously. But this interpretation merely shifts the question to "Why do I find myself experiencing the branch/world with the spot here and not the branch/world with the spot there?" ("Decoherence does not get rid of the quantum paradox", Nature 453, 978-979 (19 June 2008))