Fredrik said:
I have no idea what this is supposed to mean. |\psi(x,t)|^2 is the probability density of finding the particle in a region of space near x at time t. If it isn't, it isn't QM.
Yes, it is. You said in your earlier post that interpretations of QM don't matter - now you're saying the opposite. What I'm saying here is just the standard mathematics with a perfectly standard hidden variables interpretation.
The Schrödinger equation of 1926 is set up
as if particles existed all the time (wave function depends on position of all the particles, the Hamiltonian has Coulomb interactions between point particles etc.). De Broglie set up his pilot-wave hidden variables theory of 1924-1927 along those lines - there were particles, and the Schrödinger wave 'guided' the particles as they move along the streamlines of the probability flow which explains the double slit experiment. Note the whole concept of a wave function was de Broglie's in the first place - using it to predict electron diffraction through a slit was what he got the Nobel prize for.
(Note that this is mathematically identical to what is normally called Bohmian mechanics or the Bohm interpretation - all Bohm did was add decoherence to de Broglie's original pilot wave theory in order to explain measurement).
So anyway, in a spirit of positivism fashionable at the time, Heisenberg and the others then claimed that particles didn't exist unless you measure them. So they then changed the meaning of the word probability to mean 'probability of finding the particle at point x in a suitable position measurement' instead of its original meaning of 'probability of the particle being at x'. This leads to essentially all the features of QM that are normally considered paradoxical, but that's by the by. This is the
only difference between the standard QM viewpoint and the hidden variables viewpoint. It's the same mathematics, different interpretation.
In presentations of de Broglie-Bohm theory, it's normally said that there is an extra equation - the guidance equation - where the velocity is given by v = grad S, where S is the phase of the Schrödinger wave. In fact this is just the ordinary probability current over the density from the standard theory - again, the particles are following the streamlines of probability flow.. So there isn't an extra equation at all.
If you believe that particles and waves are logically separate entities then their distribution in space does not have to have any relation to each other. However, because the wave guides the particles then there is a natural 'equilibrium distribution' analagous to the ones in classical stat mech. That equilibrium distribution is found (by numerical simulations, or by maths) to be the square of the wave function. Now in standard QM the relation 'probability = psi^2' is simply given, with no reason or explanation - in hidden variables theories it has a causal explanation.
In extreme conditions (the early universe for example) it is postulated - see papers by Antony Valentini ,for example - that one can find non-equilibrium matter where p is not equal to psi^2, in which case non-local signalling becomes possible, as I've already stated.
This may sound like nutter stuff to you, but it's perfectly standard. You've just been conditioned to think from a positivist viewpoint just like Bohr told you to (note the view isn't even correctly applied here, as it is the wave function which is not measurable; the particle positions are!).
Anyway, given that such signalling is possible (i.e. in theory, ignoring practical problems) one then must consider the implications of instantaneous signalling for the ontology of space and time, which I believe is the point of this discussion.
Remember again, it
is standard QM. If you don't believe that, you need to do some reading.
Zenith