[ExI] Bell's Inequality
Jason Resch
jasonresch at gmail.com
Thu Dec 1 17:41:01 UTC 2016
On Thu, Dec 1, 2016 at 10:24 AM, Stuart LaForge <avant at sollegro.com> wrote:
> Jason Resch wrote:
> <Are you familiar with:
> https://en.m.wikipedia.org/wiki/Compatibilism ?
> [...]
> I am a compatibilist when it comes to freewill and determinism.>
>
> Thanks for the link, I will look into it.
>
> Jason Resch wrote:
> <Someone earlier stated Bell's Inequality implies we have to give up one
> of: locality, determinism, or realism. This list is incomplete, we must
> give up one of: locality, determinism, realism, or counterfactual
> definiteness.
> Counterfactual definiteness means experiments have only one outcome. MWI
> gives up counterfactual definiteness and retains locality, determinism and
> realism.>
>
> My understanding of counterfactual definiteness is that it is very
> specific type of realism. It is the notion that objects have measurable
> properties that have a definite value even if measurements are not made.
>
> For example, whenever you list your weight on a driver's license
> application without weighing yourself beforehand, you are assuming a
> counterfactual definiteness to your weight. Even if you were off by a few
> pounds, the idea is that if you were to weigh yourself, you would measure
> a certain weight and that's how much you actually weigh even if you didn't
> bother weighing yourself.
>
> If you give up counterfactual definiteness, it means you don't have a
> weight when you are not standing on a scale. So I am not sure what you
> mean by saying that "MWI gives up counterfactual definiteness".
>
It is giving up the part that only one possible result will be measured for
a particular value. I would point you towards this explanation for question
32 from the many worlds FAQ (
http://www.anthropic-principle.com/preprints/manyworlds.html ):
The decomposition into four worlds is forced and unambiguous after
communication with the remote system. Until the two observers
communicated their results to each other they were each unsplit by each
others' measurements, although their own local measurements had split
themselves. The splitting is a local process that is causally
transmitted from system to system at light or sub-light speeds. (This
is a point that Everett stressed about Einstein's remark about the
observations of a mouse, in the Copenhagen interpretation, collapsing
the wavefunction of the universe. Everett observed that it is the mouse
that's split by its observation of the rest of the universe. The rest
of the universe is unaffected and unsplit.)
When all communication is complete the worlds have finally decomposed
or decohered from each other. Each world contains a consistent set of
observers, records and electrons, in perfect agreement with the
predictions of standard QM. Further observations of the electrons will
agree with the earlier ones and so each observer, in each world, can
henceforth regard the electron's wavefunction as having collapsed to
match the historically recorded, locally observed values. This
justifies our operational adoption of the collapse of the wavefunction
upon measurement, without having to strain our credibility by believing
that it actually happens.
To recap. Many-worlds is local and deterministic. Local measurements
split local systems (including observers) in a subjectively random
fashion; distant systems are only split when the causally transmitted
effects of the local interactions reach them. We have not assumed any
non-local FTL effects, yet we have reproduced the standard predictions
of QM.
So where did Bell and Eberhard go wrong? They thought that all theories
that reproduced the standard predictions must be non-local. It has been
pointed out by both Albert [A] and Cramer [C] (who both support
different interpretations of QM) that Bell and Eberhard had implicity
assumed that every possible measurement - even if not performed - would
have yielded a *single* definite result. This assumption is called
contra-factual definiteness or CFD [S]. What Bell and Eberhard really
proved was that every quantum theory must either violate locality *or*
CFD. Many-worlds with its multiplicity of results in different worlds
violates CFD, of course, and thus can be local.
Thus many-worlds is the only local quantum theory in accord with the
standard predictions of QM and, so far, with experiment.
[A] David Z Albert, _Bohm's Alternative to Quantum Mechanics_
Scientific American (May 1994)
[As] Alain Aspect, J Dalibard, G Roger _Experimental test of Bell's
inequalities using time-varying analyzers_ Physical Review Letters
Vol 49 #25 1804 (1982).
[C] John G Cramer _The transactional interpretation of quantum
mechanics_ Reviews of Modern Physics Vol 58 #3 647-687 (1986)
[B] John S Bell: _On the Einstein Podolsky Rosen paradox_ Physics 1
#3 195-200 (1964).
[E] Albert Einstein, Boris Podolsky, Nathan Rosen: _Can
quantum-mechanical description of physical reality be considered
complete?_ Physical Review Vol 41 777-780 (15 May 1935).
[S] Henry P Stapp _S-matrix interpretation of quantum-theory_ Physical
Review D Vol 3 #6 1303 (1971)
There is also this article which seems to cover exactly the subject at
hand: https://arxiv.org/pdf/0902.3827.pdf
> My biggest concern with MWI is that it requires the Universal Wave
Function to be objectively real, not merely a mathematical abstraction. So
> if the UWF is objectively real then that means the infinite-dimensional
> Hilbert space that describes it is objectively real. So where is this
> gigantic Hilbert space hiding? Why do we only perceive 3+1 dimensions in a
> multiverse controlled by an infinite dimensional Wave Function? What is
> the relationship of our percievable space-time to the Universal Wave
> Function and the Hilbert space in which It dwelleth?
>
The wave function is a standard assumption of all QM
theories/interpretations that accurately describes the evolution of any
isolated system. The *universal* wave function just treats the entire
universe as an isolated system, and applies the regular rules of QM to
determine how it evolves.
Jason
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