Demystifier said:
OK, it is local for you. But is it local for itself? Is the whole Universe (the collection of All worlds of mwi) local? Is the split/branching of the Universe in a number of different copies a local event? And if you say that this question is irrelevant, isn't such a view of nature quite antropomorphic?
"The whole universe" in MWI is nothing else but the state vector, which evolves under unitary evolution. So the question of locality is related to this unitary evolution. It doesn't need to be so. For instance, the unitary evolution induced by, say, the Coulomb hamiltonian in NR QM certainly doesn't induce a local unitary evolution (in the same way as the Coulomb force in classical phase space doesn't induce a local phase flow, given that there is "action at a distance"). But if the interactions in the hamiltonian (which is the generator of unitary evolution) are local, then the unitary flow in Hilbert space is just as local as the phase space flow in classical mechanics, if the interactions are local. This can easily be verified by the fact that this unitary evolution can be written out in a Lorentz-invariant way.
The "splittings in worlds" in MWI is a pure observer-dependent concept: not for all observers, the universe is "split" in the same way. In fact, this splitting is simply the projection on the different "subspaces of awareness" by the observer (that is, those subspaces of hilbert space which correspond to different "states of awareness", which you can grossly imagine to correspond to different memory states which correspond to "observations"). "Worlds" do not have any objective ontological existence in MWI, independent of an observer.
Look at the wavefunction, where Alice has done a measurement and Bob has done a measurement, but they didn't talk to each other yet:
|psi> = |alice+> (u |bob+> + v|bob->) + |alice->(w |bob+> + x |bob->)
For Alice, there are 2 worlds, one in which she has seen the + outcome, and one in which she has seen the - outcome. Her local state description is |alice+> in one world, and |alice-> in another, and the |alice+> state has an overall weight of u^2 + v^2, while the |alice-> world has an overall weight of w^2 + x^2.
Note that these elements are in no way affected by what happens at Bob, as long as this is a local, unitary evolution. Whatever happens to the "bob" states, the weight of the Alice+ state will always remain u^2 + v^2.
We can re-write the SAME state vector from Bob's PoV:
|psi> = |bob+>(u |alice+> + w |alice-> + |bob-> (v |alice+> + x |alice->)
For Bob, there are also 2 worlds, one in which he has seen the + outcome, and one in which he has seen the - outcome. The bob+ state has an overall weight of u^2 + w^2 and the bob- state has an overall weight of v^2 + x^2.
Again, this local state description of Bob is independent of what happens at Alice: the weights of these two states will remain the same under any unitary transformation at Alice's place.
Note also that Alice's worlds have nothing to do with Bob's worlds.
Now, imagine they come together, and exchange their information. This alters of course the "state of awareness" for both alice and bob, but can only occur when they are in local contact.
We now have an evolved state:
|psi2> = u|bob++> |alice++> + w |bob+->|alice-+> + v|bob-+>|alice+-> + x |bob-->|alice-->
We now have an altered state for alice, which can be in 4 different states:
alice++, alice+-, alice-+ and alice--, with weights respectively u^2, v^2, w^2 and x^2.
This modification of alice's state description came about because of her LOCAL interaction with Bob, when he came to tell her his results. The unitary evolution which did this was local to the place of meeting.
Alice now lives in 4 worlds (and so does bob), and this time the worlds coincide between alice and bob (because they are in local interaction).
Notice the difference with a projection-based (and hence non-local) explanation of this story:
Before Alice or Bob performs a measurement, the state is:
|psi> = |alice0> (|a+>(u |b+> + v|b->) + |a->(w |b+> + x |b->)) |bob0>
(where we introduced the a-states, of the particle at Alice's place,and the b-states, of the particle at Bob's place).
Alice's weight is 1 for her state alice0.
However, the weight for the a+ state (at Alice's place) is (u^2 + v^2) while the weight for the a- state (at Alice's place) is (w^2 + x^2)
Let us first say that Bob performs a measurement, and his outcome is +:
this MODIFIES the statevector by projection:
|psi'> = |alice0> (|a+>(u |bob+>) + |a->(w |bob+>))/sqrt(u^2 + w^2)
and note that this CHANGES the weights of the a-states at Alice:
instead of a weight u^2 + v^2, we now have a weight of u/sqrt(u^2 + w^2) for the a+ state, and a weight w/(sqrt(u^2 + w^2) instead of (w^2+x^2) for the a- state.
So we see here that a state description of something at ALICE has been changed by a remote interaction (Bob's measurement). This is what is non-local in the projection postulate. It is the essence of the EPR effect.
Alice's state description has not been altered however. But of course, as Alice is going to interact locally with a, she will find a different state now than if Bob wouldn't have measured (with projection) on his side.
Alice's measurement will do nothing special to Bob's: imagine she finds +:
|psi"> = |alice+>|bob+>
This interaction doesn't do anything "non-local". Bob's state was +1 with weight 1, and this remains so. The culprit was the first measurement by bob, who ALTERED the state description of the a-particle remotely, by projection. This is the explicit non-local mechanism in "standard" projection-based quantum mechanics. Mind you that what introduces the alteration of the local state description is the projection: the fact of throwing away some terms in the wavefunction for ALL constituents, local or remote. The unitary evolution cannot do such a thing (if the interactions in it are local), because there is conservation of hilbert norm.