On 08 Nov 2014, at 19:43, John Clark wrote:

On Sat, Nov 1, 2014 at 6:55 PM, Bruce Kellett <[email protected] > wrote:

  > MWI struggles to explain the violations of Bell's inequality.

The Many world's interpretation easily explains the violation of Bell's inequality;

I think Bruce was saying that the MW struggles to explain the Bell's inequality in a local way.

I disagree with Bruce, in the sense that I take QM, that is the verifiable interference of all terms of the waves, as a strng evidence that what is real is the configuration space (at least in the first approximations). Then the universal wave (meaning by this the wave describing both the physicists and the particles observed) explains the Bell's inequality verification in the (first person plural) diaries of the persons involved in an Aspect-like experience on entangled qubit.

From a physical points of view, everything acts locally everywhere, and the non-locality exists only because the "final" observers are themselves entangled with particular terms of the waves.

It is instructing to look at teleportation in the MWI. You see that at the end, when Alice give a *classical* phone cone to Bob, she just tell him in which of the four branches of the final superposition she is, in the classical starting qubit base. In other bases, you get the same proportion of Alice, but wtih a multiple of 4 (could be 4 * infinity, also, as the position plays some role here.

That is why also, I agree with Deutsch that "soplliting universe" is not a good picture. It is really just the equality of the tensor product which is at play.

You X 1/sqrt(2)(up + down) = 1/sqrt(2)(you X up + you X down), even if you don't look at the particle. (With "you" being anything you want). If you decide to look at the particle up V down state, you only differentiate, and that is a local phenomenon, but it is contagious to anything you interact with, and 8 minutes latter, the sun itself interact, so that if you want to see the particles in the superposition state, you will need to make the sun no more recording the facts, which will be very hard, as the sun is very hot.


It is the same with the EPR-Bohm singlet state 1/sqrt(2) (up down - down up), but as Bruce points out, and I think you would agree with him, it is not that clear. Yopu have to realize that in the MW picture, that state describes an infinity of of worlds with all the(1/ sqrt(2)() up' down' - up' down' ). In this case avoidng the relative proportion of histories from the two worlds apparently invoked in the singlet expression does not work, and that give the feeling that we loose locality, even in the Many world. So, the quantum is not coherent with locality if we take the MW picture too much naively. The "truth" here, again, is in the configuration space, where the universal vector rotates.





yes the explanation is weird but any successful theory would have to be weird because Quantum Mechanics is weird.

Weird, but if we assume computationalism, then it is not so weird, in the sense that something like QM should be expected. If we assume computationalism, there is a level where we are emulated by the infinitely many relations, which are true independently of us, in the smae sense that "17 is p^rime" is true independently of you or me. This implies that whatever we find below the substitution level, it involves an infinite sum on all computations. The math explains then where the linear and the symmetries comes from, and how "consciousness", even in the weak sense of first person reports of experiences, break the symmetries, and makes the antisymmetric appearances of the subjective experience.



Unlike General Relativity no same person would come up with Quantum Mechanics unless forced to do so do to experimental results.

With the exception of those trying to understand consciousness, when taking seriously the computationalist hypothesis in the cognitive science. It leads to a measure problem, and the math indicates already that QM is a solution of that problem. But it remains to verify it is the unique solution of the math problem in arithmetic. Then we will gain the conceptual apparatus to see what are really quanta, and what are "only" qualia.



Common sense tells us that Bell's inequality can never be violated, but common sense is dead wrong.

Yes,. Note that common sense is all we have, to understand that common sense can be dead wrong. But computationalism does not need empirical facts to predict a many- dream-states-histories-worlds structure for the realm of the observable.

Of course you need step 3-7, at least, and it is even better with step 3-8. (in the Universal Dovetailer Argument (UDA).



> It can do so only in a very strained way, and that at the price of counterfactual definiteness. It seems to me that this price might be too high.

But it's even worse for the conventional Copenhagen interpretation, it says that a electron's position and momentum aren't just unknown they don't even exist until somebody looks at it, and if you look at it in such a way that you can determine it's position then it's meaningless to ask what it's momentum would have been if you'd measured that instead. Many worlds says that the electron always had a real position and momentum but when you (and by "you" I mean the only thing the laws of physics lets third parties see that fits the description of Bruce Kellett) measure the electron the universe splits,

It is just you who differentiate, and I let you as exercise to introduce the 1p / 3p nuance to make that "you" non ambiguous. If you can do that, you can move at step 4, which explains at least why if our body are machine, then below the substitution level, matter get a little (qu)bit bezerk.



in one universe "you" measure the electron's position and in the other universe "you" measure the electron's momentum, and although they (the 2 yous) can't communicate with each other both are equally real. So if you're a fan of counterfactual definiteness you should be a fan of Many Worlds too.

I think so, but I have not yet a good picture of Kochen and Specker paradox in the MWI. Might say more later. Paper by Hardegree, also discussion with Russell Standish around the movie graph argument (step 8), confirms my feeling that quantum logic (and the []p & <>t, [] & <>t & p logics) defines a logic of the conditional/counterfactual. I expect also that counterfactual definiteness lover should feel more at ease with the MW than with Copenhagen. OK.

Bruno




  John K Clark


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