On Thu, Jan 2, 2014 at 11:44 AM, Edgar L. Owen <[email protected]> wrote:

> Jason,
>
> No, please carefully read my new topic post "Another shot at how spacetime
> emerges from quantum events"
>

Okay.

Just as a tip, which I think will make  things a little easier for others
to follow a conversation, is to generally it is best to answer new
questions within the same thread where the question is asked, and ideally
with responses in-line with the question. This is the usual convention on
this list.  To be clear, I think it is fine to say "I've already answered
question X in thread Y", but if it is a new question in thread Z, it is
probably better to answer it in thread Z.

This is particularly true as it is common for a single thread to grow to
include dozens, if not hundreds of responses, and locating the answer in
that thread can become very difficult.


> where I explain this process in detail. You will see why it doesn't lead
> to MW but instead to many fragmentary spacetimes (entanglement networks)
> which link and align via shared events. But all this occurs in the same
> underlying computational (not dimensional) space which everything is part
> of.
>
> The spin orientation of the two particles is fixed in their mutual frame
> when they are created. It's just that that frame (entanglement network) is
> not linked to that of the observer until a common event (observer's
> measurement of one particle's spin) links and aligns the particles' spin
> orientation frame to that of the observer's. Prior to that they are
> completely separate spacetimes. That's why the spins are indeterminate in
> the frame of the observer until he measures one and by doing so links and
> aligns their frame with his.
>
> This process falsifies FTL, non-locality, MWI (unless you want to call the
> fragmentary entanglement networks separate worlds. They are separate
> spacetime fragments but not really separate 'worlds' since they continually
> merge and align at common events in the SAME computational reality.)
>
>
But the point I and others have repeatedly made is that this is a local
hidden variable theory, which is unworkable without FTL influences (given
Bell's theorem, which is a mathematical proof).

Jason


> Edgar
>
> On Thursday, January 2, 2014 9:11:57 AM UTC-5, Jason wrote:
>
>>
>>
>>
>> On Thu, Jan 2, 2014 at 7:53 AM, Edgar L. Owen <[email protected]> wrote:
>>
>>> Jason,
>>>
>>> Great! An amazing post! You seem to have correctly gotten part of the
>>> theory I proposed in my separate topic "Another stab at how spacetime
>>> emerges from quantum events." Please refer to that topic to confirm...
>>>
>>> Do you understand how the fact that the spins are determined in the
>>> frames of the spinning particles WHEN they are created falsifies FTL and
>>> non-locality?
>>>
>>
>> Yes, but I also think this leads to many worlds, since there is not a
>> single state of the superposition. The particle pair is not just Up_Ddown
>> or Down_Up, but both Up_Down + Down_Up. After the measurement, it is
>> Measured_Up_Down + Measured_Down_Up.
>>
>> Bell's inequality leads to a refutation that the two particles can have
>> just a single state.
>>
>> Jason
>>
>>
>>>
>>> Edgar
>>>
>>>
>>>
>>> On Wednesday, January 1, 2014 2:21:33 PM UTC-5, Jason wrote:
>>>>
>>>>
>>>>
>>>>
>>>> On Wed, Jan 1, 2014 at 4:33 AM, LizR <[email protected]> wrote:
>>>>
>>>>> On 1 January 2014 21:34, meekerdb <[email protected]> wrote:
>>>>>
>>>>>>  On 12/31/2013 7:22 PM, LizR wrote:
>>>>>>
>>>>>>  On 1 January 2014 13:54, meekerdb <[email protected]> wrote:
>>>>>>
>>>>>>>  Of course in Hilbert space there's no FTL because the system is
>>>>>>> just one point and when a measurement is performed it projects the 
>>>>>>> system
>>>>>>> ray onto a mixture of subspaces; spacetime coordinates are just some 
>>>>>>> labels.
>>>>>>>
>>>>>>
>>>>>>  I thought there was no FTL in ordinary space, either? (I mean, none
>>>>>> required for the MWI?)
>>>>>>
>>>>>> Right, but the state in Hilbert space is something like |x1 y1 z1 s1
>>>>>> x2 y2 z2 s2> and when Alice measures s1 at (x1 y1 z1) then s2 is 
>>>>>> correlated
>>>>>> at (x2 y2 z2).  As I understand it the MWI advocates say this isn't FTL
>>>>>> because this is just selecting out one of infinitely many results |s1 
>>>>>> s2>.
>>>>>> But the 'selection' has to pair up the spins in a way that violates 
>>>>>> Bell's
>>>>>> inequality.
>>>>>>
>>>>>
>>>>> If I understand correctly ... actually, let me just check if I do,
>>>>> before I go any further, in case I'm talking out my arse. Which wouldn't 
>>>>> be
>>>>> the first time.
>>>>>
>>>>> I assume we're talking about an EPR correlation here?
>>>>>
>>>>> If yes, I've never understood how the MWI explains this.
>>>>>
>>>>
>>>> The thing to remember is entanglement is the same thing as measurement.
>>>>  The entangled pair of particles have measured each other, but they remain
>>>> isolated from the rest of the environment (and thus in a superposition, of
>>>> say UD and DU). Once you as an observer measure either of the two
>>>> particles, you have by extension measured both of them, since the position,
>>>> which you measured has already measured the electron, and now you are
>>>> entangled in their superposition.
>>>>
>>>> Jason
>>>>
>>>>
>>>>
>>>>>  I've see it explained with ASCII diagrams by Bill Taylor on the FOAR
>>>>> forum, and far be it from me to quibble with Bill, but it never made sense
>>>>> to me. Somehow, the various branches just join up correctly...
>>>>>
>>>>> The only explanation I've come across that I really understand for
>>>>> EPR, and that doesn't violate locality etc is the time symmetry one, where
>>>>> all influences travel along the light cone, but are allowed to go either
>>>>> way in time.
>>>>>
>>>>> So although I quite like the MWI because of its ontological
>>>>> implications, this is one point on which I am agnostic, because I don't
>>>>> understand the explanation.
>>>>>
>>>>>>
>>>>>>
>>>>>>      In fact, it's generally assumed to be very, very STL (unless
>>>>>>> light itself is involved). At great distances from the laboratory, one
>>>>>>> imagines that the superposition caused by whatever we might do to cats 
>>>>>>> in
>>>>>>> boxes would decay to the level of noise, and fail to spread any further.
>>>>>>>
>>>>>>>  That's an interesting viewpoint - but it's taking spacetime instead
>>>>>>> of Hilbert space to be the arena.  If we take the cat, either alive or
>>>>>>> dead, and shoot it off into space then, as a signal, it won't fall off 
>>>>>>> as
>>>>>>> 1/r^2.
>>>>>>>
>>>>>>>  No, but it will travel STL!
>>>>>>
>>>>>>
>>>>>> Sure.  I was just commenting on the idea that the entanglement has a
>>>>>> kind of limited range because of 'background noise'.  An interesting 
>>>>>> idea,
>>>>>> similar to one I've had that there is a smallest non-zero probability.
>>>>>>
>>>>>> But if you want to get FTL, that's possible if Alice and Bob are near
>>>>>> opposite sides of our Hubble sphere when they do their measurements.  
>>>>>> They
>>>>>> are then already moving apart faster than c and will never be able to
>>>>>> communicate - with each other, but we, in the middle will eventually
>>>>>> receive reports from them so that we can confirm the violation of Bell's
>>>>>> inequality.
>>>>>>
>>>>>
>>>>> Hmm, that's a good point. That would, however, fit in nicely with time
>>>>> symmetry (which really needs a nice acronym, I'm not sure "TS" cuts it). I
>>>>> tend to evangelise a bit on time symmetry, but only because everyone else
>>>>> roundly ignores it, and it seems to me that it at least has potential.
>>>>>
>>>>>
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