kvantti said:
Actually the paths satisfy the Heisenberg uncertainty relation between momentum and position.
The uncertainty principle does not allow momentum conservation violations, it only limits predictability. If MWI is a realistic interpretation you cannot have multiple paths for the same particle unless its momentum can change at random.
Also, all the possible paths affect the observed position of a particle in the double slit experiment, for example. If the paths are unphysical, how can they affect the observed positions of the particles?
A particle can only change momentum if a force is acting on it (because momentum conservation). In a double slit experiment for example the path of the particle is determined by the interactions between the particle and the charged particles in the wall (electrons and quarks), therefore it depends on the geometry of the wall. But it is possible to describe the same geometry by referring not to the places where there are charges but to the places where there is no charge (the paths you are referring). But this is only a method to make the calculations. The true reason for particle's trajectory stands in its EM interaction with other particles.
ueit said:
QM just doesn't say anything about the stochastic/deterministic nature of the events it describes.
Again, you can interpret it does.
Sure you can, but the burden of proof is on you to show that such an interpretation is inevitable unless MWI is employed.
Every stochastic/non-local/indeterministic interpretation does contradict relativity. This has more to do with metaphysics than actual physics but you can't fit a model which is interpreted as being indeterministic with a model that is interpreted as being deterministic.
This is a good reason to reject such interpretations. However, this doesn't mean MWI wins by default. There is another possibility, that QM is incomplete and, just like thermodynamics, it is only a statistical description of a classical world.
The wavefunction doesn't actually tell the whole story; path integral formulation gives a more fundamental insight about the behavior of particles. You should read Feynmans QED: strange theory of light and matter if you haven't. I got shocked many times when reading it because you get so confused about how the nature works. Don't worry, there's no mention about the MWI.
I see no good reason to believe that "path integral formulation gives a more fundamental insight about the behaviour of particles". It is just another way to do calculations.
I've read Feynman's book about a year ago, so it's not that fresh into my memory but I don't remember him claiming that the path integral is a realistic description of how nature works.
I have nothing against MWI, it's just as good as the other QM interpretations. It may even be true but we'll never know it, because it's unfalsifiable. The assumption that QM is a complete description has to be challenged first.
Nope, it is a classical theory. Only stochastic particles (that exist in the indeterministic interpretations of QM) contradict relativity.
One could produce a fundamentally stochastic interpretation of thermodynamics as well. So what? I agree with you that any stochastic theory contradicts relativity but I disagree that QM is inherently stochastic or that MWI is the only way QM could be deterministic.
How does it contradict my original assumption? According to MWI, the statefunction/wavefunction is a statistical tool that describes the relative states of a single particle in different parts of the multiverse, ie. it describes the distribution of the particles position in different universes.
QM is defined on a Newtonian (or Minkowsky for QFT) background. One universe, three spatial dimensions, one time dimension. Where are these other universes coming from? They do not appear in the initial description of the system.
In the MWI FAQ you linked I read:
Loosely speaking a "world" is a complex, causally connected, partially or completely closed set of interacting sub-systems which don't significantly interfere with other, more remote, elements in the superposition. Any complex system and its coupled environment, with a large number of internal degrees of freedom, qualifies as a world.
I admit I don't understand anything from this definition. There is no such thing as an isolated system (except the universe as a whole) and what is "significant" is a matter of opinion. Just because a force is weak doesn't mean it's not significant.
You can calculate the probability of the cat being alive at a time [t] by remembering that the probability of finding the cat alive after Δt=[half-life of the nucleus] is 50%, so after Δt=n*[half-life of the nucleus] the probability of finding the cat alive is (0.5)^n.
I know that, done in chemistry classes. I don't see where MWI is used here though.
Clive Price's MWI FAQ said:
How many worlds are there?
The thermodynamic Planck-Boltzmann relationship, S = k*log(W), counts the branches of the wavefunction at each splitting, at the lowest, maximally refined level of Gell-Mann's many-histories tree. (See "What is many-histories?") The bottom or maximally divided level consists of microstates which can be counted by the formula W = exp (S/k), where S = entropy, k = Boltzmann's constant (approx 10^-23 Joules/Kelvin) and W = number of worlds or macrostates. The number of coarser grained worlds is lower, but still increasing with entropy by the same ratio, i.e. the number of worlds a single world splits into at the site of an irreversible event, entropy dS, is exp(dS/k). Because k is very small a great many worlds split off at each macroscopic event.
So, how do you apply this convoluted explanation to Schrödinger’s cat?
If a particle is in a superposition of states, say |x1> + |x2>, and you observe the particles state, then the universe is split in two: in one universe you observe the particles state being as |x1> and in the other |x2>. This is sufficient enough to distinguish two universes as being "different".
Is world splitting related to observation, like the "collapse" in Copenhagen interpretation or a real, physical event?