On Wednesday, April 25, 2018 at 10:51:13 AM UTC, Bruce wrote:
>
> From: Bruno Marchal <[email protected] <javascript:>>
>
> On 22 Apr 2018, at 01:47, Bruce Kellett < <javascript:>
> [email protected] <javascript:>> wrote:
>
> From: smitra <[email protected] <javascript:>>
>
>
> On 22-04-2018 00:18, Brent Meeker wrote:
>
>> On 4/21/2018 12:42 PM, smitra wrote:
>>
>>>
>>> That's then an artifact of invoking an effective collapse of the 
>>> wavefunction due to introducing the observer. The correlated two particle 
>>> state is either put in by hand or one has shown how it was created. In the 
>>> former case one is introducing non-local effects in an ad-hoc way in a 
>>> theory that only has local interactions, so there is then nothing to 
>>> explain in that case. In the latter case, the entangled state itself 
>>> results from the local dynamics, one can put ALice and Bob at far away 
>>> locations there and wait until the two particles arrive at their locations. 
>>> The way the state vectors of the entire system that now also includes the 
>>> state vectors of Alice and Bob themselves evolve, has no nontrivial 
>>> non-local effects in them at all.
>>>
>>
>> Sure it does.  The state vector itself is a function of spacelike
>> separate events, which cause it to evolve into orthogonal
>> components...whose statistics violated Bell's inequality.
>>
>> Brent
>>
>
> There is no non-locality implied here unless you assume that the dynamics 
> as predicted by QM is the result of a local hidden variables theory.
>
> Saibal
>
>
> There is no need to suggest local (or non-local) hidden variables. The 
> non-locality we are talking about is implied by the quantum state itself -- 
> nothing to do with the dynamics.
>
>
>
> But that type of non-locality has never been questioned, neither in the 
> MWI, or a fortiori in QM+collapse. But the MWI explains without the need of 
> “mysterious” influence-at-a-distance, which would be the case in the 
> mono-universe theory, or in Bohm-De Broglie pilot wave theory. Without 
> dynamic we have “only” d’Espagnat type of inseparability.
>
> Bruno
>
>
> It seems that you are starting to see it from my perspective. Non-locality 
> is just another way of emphasizing the non-separablity of the quantum 
> singlet state. As you say, this is true in MWI as in collapse theories. In 
> my extended development of the mathematics in another recent post, I 
> demonstrated that there is actually no difference between MWI and CI in 
> this regard. All that we have is the non-separability of the state, which 
> means that a measurement on one particle affects the result of measurements 
> on the other -- they are inseparable. This is all that non-locality means, 
> and this is not changed by MWI. An awful lot of nonsense has been talked 
> about this -- people trying to find a "mechanism" for the inseparability -- 
> but that is not necessary. Quantum theory requires it, and it has been 
> totally vindicated by experiment. That is the way things are, in one world 
> or many.
>
> Bruce
>

You place great faith in the singlet wf. But how can you legitimately treat 
the system quantum mechanically if you assume zero uncertainty in the total 
spin AM? AG

-- 
You received this message because you are subscribed to the Google Groups 
"Everything List" group.
To unsubscribe from this group and stop receiving emails from it, send an email 
to [email protected].
To post to this group, send email to [email protected].
Visit this group at https://groups.google.com/group/everything-list.
For more options, visit https://groups.google.com/d/optout.

Reply via email to