On Thu, Jan 2, 2014 at 10:59 AM, Bruno Marchal <[email protected]> wrote:

>
> On 02 Jan 2014, at 15:11, Jason Resch 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.
>
>
> I agree with what you *mean*, but it is pedagogically confusing to say it
> in that way.  Up+Down *is* a single state (in the complementary base).
> A bag of Up+Down particles behaves differently than a mixture of Up and
> Down particles.
>
>
>
Thanks, I will be sure to make that point more explicit in the future.


>
>
> The particle pair is not just Up_Ddown or Down_Up,
>
>
> Indeed that would be the case of a particle taken in the second bag:
> the mixture of Up-down and Down-up pairs of particles.
>
>
>
> 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.
>
>
> I understand what you mean, but Measured_Up_Down + Measured_Down_Up is a
> single superposed state, which is indeed the result of the linearly
> contagion of Up_Down + Down_Up to the one of the observer. With the
> universal wave of Everett, there is only one pure quantum state, and it is
> perhaps the vacuum state (H=0) which is the superposition of all possible
> complementary states of the universe.
>
> In set theory there is something analogous. if you define the unary
> intersection INT(x) by the intersection of all y in x, you have that the
> INT({ }) = the set theoretical universe, that is the class of all sets
> (which is usually not a set in the most common set theories). It is similar
> to a^0 = 1.
>
>
I think I was following until you said it is like a^0 = 1..

Jason


>
> With comp, there is not even such a wave, and I prefer to put the sets in
> the numbers' epistemology. The wave has to be what the average universal
> machine observes when it looks below its substitution level relatively to
> its most probable computations/universal neighbor.
>
> Why does the quantum wave win the measure battle? I think the explanation
> is in the "material", probabilistic, intensional nuance of self-reference.
>
> Bruno
>
>
>
> 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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>>>
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> http://iridia.ulb.ac.be/~marchal/
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