On Sunday, November 26, 2017 at 8:29:22 AM UTC-6, Bruno Marchal wrote:
>
>
> On 24 Nov 2017, at 15:59, Lawrence Crowell wrote:
>
> On Thursday, November 23, 2017 at 5:53:14 PM UTC-6, Bruce wrote:
>>
>> On 24/11/2017 10:15 am, Lawrence Crowell wrote:
>>
>> On Wednesday, November 22, 2017 at 9:37:48 AM UTC-6, Bruno Marchal wrote: 
>>>
>>>
>>> On 20 Nov 2017, at 23:04, Bruce Kellett wrote:
>>>
>>>
>>> You clearly have not grasped the implications of my argument. The idea 
>>> that "MWI replaces all nonsensical weirdness by one fact (many histories)" 
>>> does not work, and is not really an explanation at all -- you are simply 
>>> evading the issue.
>>>
>>>
>>> Without collapse, the apparent correlations are explained by the linear 
>>> evolution, and the linear tensor products only. I have not yet seen one 
>>> proof that some action at a distance are at play in quantum mechanics, 
>>> although I agree that would be the case if the outcome where unique, as 
>>> EPER/BELL show convincingly.
>>>
>>> Aspect experience was a shock for many, because they find action at a 
>>> distance astonishing, but are unaware of the many-worlds, or just want to 
>>> dismiss it directly as pure science fiction. But after Aspect, the choice 
>>> is really between deterministic and local QM + many worlds, or one world 
>>> and 3p indeterminacy and non locality. Like Maudlin said, choose your 
>>> poison.
>>>
>>>
>>> Bruno
>>>
>>> Bruce
>>>
>>>
>> I am new to this list and have not followed all the arguments here. In 
>> weighing in here I might be making an error of not addressing things 
>> properly. 
>>
>> Consider quantum entanglements, say the entanglements of two spin 1/2 
>> particles. In the singlet state |+>|-> + |->|+> we really do not have the 
>> two spin particles. The entanglement state is all that is identifiable. The 
>> degrees of freedom for the two spins are replaced with those of the 
>> entanglement state. It really makes no sense to talk about the individual 
>> spin particles existing. If the observer makes a measurement that results 
>> in a measurement the entanglement state is "violently" lost, the 
>> entanglement phase is transmitted to the needle states of the apparatus, 
>> and the individual spin degrees of freedom replace the entanglement. 
>>
>> We have some trouble understanding this, for the decoherence of the 
>> entangled state occurs with that state as a "unit;" it is blind to any idea 
>> there is some "geography" associated with the individual spins. There in 
>> fact really is no such thing as the individual spins. The loss of the 
>> entangled state replaces that with the two spin states. Since there is no 
>> "metric" specifying where the spins are before the measurement there is no 
>> sense to ideas of any causal action that ties the two resulting spins. 
>>
>> This chaffs our idea of physical causality, but this is because we are 
>> thinking in classical terms. There are two ways of thinking about our 
>> problem with understanding whether quantum mechanics is ontic or epistemic. 
>> It could be that we are a bit like dogs with respect to the quantum world. 
>> I have several dogs and one thing that is clear is they do not understand 
>> spatial relationships well; they get leashes and chains all tangled up and 
>> if they get wrapped up around a pole they simply can't figure out how to 
>> get out of it. In this sense we human are simply limited in brain power and 
>> will never be able to understand QM in some way that has a completeness 
>> with respect to causality, reality and nonlocality. There is also a far 
>> more radical possibility. It is that a measurement of a quantum system is 
>> ultimately a set of quantum states that are encoding information about 
>> quantum states. This is the a quantum form of Turing's Universal Turing 
>> Machine that emulates other Turing machines, or a sort of Goedel 
>> self-referential process. If this is the case we may be faced with the 
>> prospect there can't ever be a complete understanding of the ontic and 
>> epistemic nature of quantum mechanics. It is in some sense not knowable by 
>> any axiomatic structure.
>>
>>
>> Hi Lawrence, and welcome to the 'everything' list. I have come here to 
>> avoid the endless politics on the 'avoid' list.
>> The issue that we have been discussing with EPR pairs is whether many 
>> worlds avoids the implications of Bell's theorem, so that a purely local 
>> understanding of EPR is available in Everettian models. I have argued that 
>> this is not the case -- that non-locality is inherent in the entangled 
>> singlet state, and many worlds does not avoid this non-locality. I think 
>> from what you say above that you might well agree with this position.
>>
>> Bruce
>>
>
> Of course MWI can do nothing of the sort. MWI suffers from much the same 
> problem all quantum interpretations suffer from. 
>
>
> I don't see this. the MW theory (that is the WWE without the collapse 
> axiom) explains the violation of inequality in a way which avoids any 
> action at a distance, but when we assume one universe, like Einstein 
> explains very clearly already in 1927, you get a notion of simultaneousness 
> incompatible with special relativity and very minimal form of realism. 
>
> For me, as a logician, I consider that SWE and SWE+collapse are different 
> theories. The first is local, deterministic and admits a local physical 
> realism, the second is not intelligible at all, as the notion of observer 
> is unclear and dualistic.
>
> Bruno
>

I suppose I don't know what WWE means. MWI is not a bad idea, but I frankly 
question whether it along with all other interpretations are properly 
scientific theories. I see no particular way that any quantum 
interpretation can be tested. The idea is nice in that it gives an idea of 
a total universe as unitary, but where the phenomenology has us moving 
along one particular path in a decoherence event. However, if we are to 
have a splitting off of the world we might think of there being a many 
block world perspective, where a decoherence of a quantum event splits off 
quantum amplitudes on all possible spatial surfaces that contain this 
event. This has been referred to in the past as the gemische; all possible 
spacelike manifolds that embed a measurement event. However, we have some 
ambiguity with respect to probability amplitudes associated with each path 
in this splitting. 

LC

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