Dmitry67 said:
Well,
http://en.wikipedia.org/wiki/Quantum_decoherence
So, after QD we have 1/2 alive cat + 1/2 dead cat. These cats don't interefere.
You have a choice: to assume that both cats do exists (Multiworlds), or to invent some new mechanism (like wavefunction collapse) to explain why the whole universe had randomly but consistently chosen one particular branch.
In that case you whould deal with the Ocamms razor (why do you need it if everything is already explained without it?) Your mechanism will be non local and you will have to answer questions like 'as QD is not immediate, at what moment the second branch dissapear? Why any particular branch is chosen? You say, randomly? What is a probability? Bayesians or Frequentisits? Why? et cetera, et cetera, et cetera...
And why? Why do you need all that weird stuff? Just because the very idea of parralel universes is so weird? because it is so easy to assume that space,or time are infinite, but for some reason we can not aqssume that WE exist in the infinite number of copies?
No after QD you have either a live cat or a dead cat with classical 50-50 probability.
The "many worlds" are many worlds of possibility. Its no different from standard classical probability. If I flip a coin I can imagine it landing heads and imagine it landing tails... two worlds in my imagination. Afterward those two worlds still exist in my imagination but I qualify one as "what might have been". I don't need a fancy mechanism or to worry about "classical probability collapse" or anything. Both "worlds" continue to "exist" in my brain.
The actual coin behaves as it behaves and I observe it as I observe it.
In order to see actual quantum behavior for cats you must first freeze the cats to near absolute zero then you'll need a very large number of frozen cats so you can do interference experiments and get a whole interference pattern. Of course the cats can't survive such an experiment so "alive vs dead" is not going to be a quantum observable anyway. Remember a cat is a heat engine and thus any quantum interaction with them by definition must decohere almost immediately.
Let me put it (decoherence) another way. Think of entropy as entanglement with the environment. (Recall that partial traces of the zero entropy joint density operator yields a non-zero entropy density operator for a partial system.) Now once a quantum system interacts with its environment it can no longer be sharply described (i.e. with a wave-function) alone. It must either be described with a density operator or to preserve the sharp description you would have to describe the system plus that part of the episystem it has interacted with and then only if that part of the episystem has been observed sharply before hand. (That is unless you have been very careful with the type of interaction i.e. you've made a measurement or are preparing the system in a sharp mode). T
You in other-words would need to observe a cross section of the system's past light-cone up to the point you still want to describe the system sharply and likewise the future light cone of that whole system. And given that bigger system has also interacted with
its environment...
If you do not do this then you introduce classical random variables into the system upon which the outcome of the future experiment on that system will depend. Thence the "collapse" of the system's wave-function is no different from the "collapse" in the expectation value for a lotto ticket once the drawing occurs, a classical probability collapse.
There is no problem to be solved by invoking Everett's many worlds. Wave function "collapse" is only a conceptual problem if you confuse the wave-function with the actual system. A lotto ticket is not the cash prize (or a superposition of many cash prizes). A wave-function is not an electron. Remember that quantum interference is more fundamental than classical wave interference. Classical waves are composites of quantum systems. Why go backwards and try to describe a quantum system as a classical wave (function)? Instead understand that the wave-function is a representation of what we know about how the system behaves.
With respect to the measurement "problem" and wave-function "collapse" consider this. The distinction between "before" and "after" is by definition separated by an environmental interaction. The variables describing the system "after" differ from those "before" said difference depending on the "in between" interaction which is necessarily probabilistic. It is not the system that suddenly changes. It is our description of the system. We choose a new wave-function because via the measurement process the system is different. The system change can be gradual or even delayed. When we interact with the measuring device our knowledge about the system changes in a classical way and we then use an updated wave-function to describe it.
Note also the intimate involvement of thermodynamics in the measurement process...(you amplify a signal and must dissipate heat into an entropy dump). Google the terms "thermodynamic" and "quantum measurement" to see what I mean. The system has changed by assumption and so its description changes by assumption and due to its interaction with a measurement device you can only describe it continuously by describing both it and the large scale variables of the measuring device which register its outcome, said variables now being highly correlated with the quantum variable of the system being measured.
The "many worlds" of Everett are "many worlds of possibility" not of reality...and what is more there are just as many of these prior to the measurement event as there are after it...they consist of the many possible configurations of the measuring device's heat dump prior to the act of measurement. You fundamentally can't describe the measuring device with a wave function due to its necessarily thermodynamic nature. It must be described at best by a density operator, classical probabilities and all. As such sequences of measurements are necessarily non-deterministic
unless your are careful about which measurements you make. No mystery, no need to puzzle over EPR experiments except to carefully avoid counterfactual hypotheses.