On Thursday, December 5, 2019 at 5:36:56 AM UTC-6, Lawrence Crowell wrote:
>
> On Thursday, December 5, 2019 at 3:43:50 AM UTC-6, Philip Thrift wrote:
>>
>>
>>
>> On Wednesday, December 4, 2019 at 6:11:25 PM UTC-6, Lawrence Crowell 
>> wrote:
>>>
>>> On Wednesday, December 4, 2019 at 4:29:03 PM UTC-6, Philip Thrift wrote:
>>>>
>>>>
>>>>
>>>> On Wednesday, December 4, 2019 at 2:31:08 PM UTC-6, Lawrence Crowell 
>>>> wrote:
>>>>>
>>>>> On Wednesday, December 4, 2019 at 1:53:39 PM UTC-6, John Clark wrote:
>>>>>>
>>>>>> On Wed, Dec 4, 2019 at 11:14 AM Lawrence Crowell <
>>>>>> goldenfield...@gmail.com> wrote:
>>>>>>
>>>>>> *>>> The entire notion of quantum states and events as localized in 
>>>>>>>>> regions of space is not entirely applicable. What symmetries exist 
>>>>>>>>> with 
>>>>>>>>> these quantum states or field are then not tied to local geometry.*
>>>>>>>>>
>>>>>>>>
>>>>>>>> >> OK, but if quantum states are to explain local geometry, and 
>>>>>>>> that is the entire point because that is all that experimenters can 
>>>>>>>> see, 
>>>>>>>> then the reverse can not be true, local geometry must be tied to 
>>>>>>>> quantum 
>>>>>>>> states. 
>>>>>>>>
>>>>>>>
>>>>>>> *> I guess this is not quite clear to me. Largely the quantum states 
>>>>>>> that form spacetime are quantum gravitation states.*
>>>>>>>
>>>>>>
>>>>>> It seems to me if quantum gravitational states form spacetime, and if 
>>>>>> spacetime is smooth and continuous as the Gamma Ray Burst evidence seems 
>>>>>> to 
>>>>>> show, then 2 distinct points that are less than a Planck Length apart 
>>>>>> must 
>>>>>> correspond to 2 distinct quantum gravitational states.  Am I wrong?
>>>>>>
>>>>>
>>>>> No it is not possible to know. If you localize a quantum bit to a 
>>>>> Planck length it is in a black hole. If you try to localize two qubits 
>>>>> arbitrarily closely they caon only be within 2 Planck areas, if on a 
>>>>> horizon,or in two Planck volumes if in the bulk. A Planck volume is V_p = 
>>>>> (4π/3)ℓ_p^3.So if you try to localize a field is less than two Planck 
>>>>> volumes, or within a length 1.26ℓ_p there is a loss of any 
>>>>> information about them.
>>>>>  
>>>>>
>>>>>>
>>>>>> >> So if the Gamma Ray Burst results hold up and spacetime really is 
>>>>>>>> smooth and continuous then, would it be correct to say there are a 
>>>>>>>> infinite 
>>>>>>>> (not just astronomically large) number of quantum symmetries and the 
>>>>>>>> Planck 
>>>>>>>> Length and the Planck Time have no physical significance, they are 
>>>>>>>> just 
>>>>>>>> numbers in units of time and space that for no particular reason 
>>>>>>>> happen to pop out when you mathematically play around with the 
>>>>>>>> constants of 
>>>>>>>> nature in certain ways?
>>>>>>>>
>>>>>>>
>>>>>>> *> The number of quantum states are Virasoro, which is in principle 
>>>>>>> infinite. However, because the cosmological horizon can only bound a 
>>>>>>> finite 
>>>>>>> number of such states, as is the case with a black hole with entropy S 
>>>>>>> = 
>>>>>>> A/4ℓ_p^2, the number of physical states is bounded above. As a result 
>>>>>>> the 
>>>>>>> Virasoro algebra has high frequency modes that are mathematically 
>>>>>>> possible, 
>>>>>>> but not physically accessed.*
>>>>>>>
>>>>>>
>>>>>> Then although mathematically infinite as far as physics is concerned 
>>>>>> there are only a finite number of quantum gravitational states, but if 
>>>>>> quantum states produces spacetime then why does the Gamma Ray Burst 
>>>>>> results 
>>>>>> say spacetime is smooth and continuous? Can 2 points that are 
>>>>>> arbitrarily 
>>>>>> close to each other have any physical meaning, does physics need Real 
>>>>>> Numbers or not?  
>>>>>>
>>>>>
>>>>> The gamma ray burst data just tells us that different wavelengths of 
>>>>> photons have no dispersion. the G(p,p') = 1/(4π(|p - p'|^2 - m^2)) 
>>>>> predicts 
>>>>> different dispersons for different wavelengths of light. Over distances 
>>>>> of 
>>>>> billions of light years this would be significant. Nothing of this sort 
>>>>> was 
>>>>> observed. This means there is no "foaminess" or discreteness to 
>>>>> spacetime. 
>>>>> This is down to a scale of ℓ_p/50, the last I checked.
>>>>>  
>>>>>
>>>>>>  
>>>>>>
>>>>>>> *> A Hilbert space H that contains H_a and H_b is not equal to 
>>>>>>> H_a×H_b. Any unitary transformation between H_a and H_b defines a 
>>>>>>> boundary 
>>>>>>> if we trace over one of these so S_a = tr_bS = -kTr_b[ρlog(ρ)] and 
>>>>>>> similarly for S_b. We have removed the off-diagonal terms. We then can 
>>>>>>> define this as a boundary, aka holographic screen or horizon, between 
>>>>>>> sets 
>>>>>>> of entangled states. This then defines a form of geometry. The 
>>>>>>> transformation between H_a and H_b can just as well be time evolution 
>>>>>>> with 
>>>>>>> a boundary that separates two temporal regions. The Taub-NUT spacetime 
>>>>>>> has 
>>>>>>> this characteristic as does the region between the spacelike region 
>>>>>>> outside 
>>>>>>> the inner horizon of a black hole and the mysterious region inside.*
>>>>>>>
>>>>>>
>>>>>> You seem to be saying space may not be fundamental but time is. Would 
>>>>>> that be a fair representation of your views?
>>>>>>
>>>>>
>>>>> I tried to indicate that both space and time are emergent.
>>>>>
>>>>> LC
>>>>>  
>>>>>
>>>>
>>>>
>>>> But everything you wrote is in the vocabulary of space+time.
>>>>
>>>> Even "wave*length"*.
>>>>
>>>> @philipthrift 
>>>>
>>>
>>> This is in reference to the propagation of photons. It illustrates that 
>>> spacetime is not made of chunks or finite elements. Spacetime is smooth. 
>>> However, it is an epiphenomenology of quantum entanglement.
>>>
>>> LC 
>>>
>>
>> How does the mathematics of *quantum entanglement* imply that *spacetime 
>> is smooth*?
>>
>> Or how does *stochastic Lorentz metric space* imply it isn't.
>>
>> The Minkowski manifold equipping the stochastic metric is referred to as 
>> the
>> stochastic Lorentz metric space (SLM-space) hereafter. A distance between 
>> two points on the SLMspace will fluctuate around the geometric distance 
>> measured by the Lorentz metric, with the distance measured by the 
>> (non-fluctuating) Lorentz metric referred here as the geometrical distance. 
>> A distribution function is required to give the geometrical distance as an 
>> average value over a two-point ensemble on the SLM-space, with the variance 
>> of the distribution function set to be proportional to its geometrical 
>> distance. This distribution function makes a null vector (vector with zero 
>> length) without any fluctuation, a desirable characteristic for restraining 
>> a null photon mass after quantum corrections. Furthermore, to satisfy the 
>> causality condition the probability changing a sign of the length of a 
>> string stretching between two points must be zero.
>>
>> https://arxiv.org/pdf/1612.04228.pdf
>>
>>
>> !philipthrift
>>
>
> As of yet the smoothness of spacetime as an emergent phenomenon is not 
> clear. However, data does not point to there being this sort of stochastic 
> processing metric. That would have had an effect that would show in the the 
> dispersion of photons from distant sources. We might think of spacetime as 
> a surface induced by the condensation of quantum states with an SU(2,2) 
> symmetry. There are then in association with this quantum states with the 
> same symmetry that are relatively separable states visa vie the condensate. 
> These are the quantum gravitational states that represent the separation 
> between an entropy surface and the horizon entropy. With Hawking radiation 
> these two surfaces converge and this leads to the condition seen in the 
> Page time.
>
> LC
>

the condensation of quantum states with an SU(2,2) symmetry
entropy surface

still merges quantum mechanics with geometrical mathematics  - which is 
what the stochastic metric  (SM) does.

And SM provides both the smoothiness of space and the probabilities of QM 
while keep ing space "real".

@philipthrift



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