On Saturday, October 5, 2019 at 4:57:10 AM UTC-5, Alan Grayson wrote:
>
>
>
> On Friday, October 4, 2019 at 4:57:30 PM UTC-6, Lawrence Crowell wrote:
>>
>> On Friday, October 4, 2019 at 7:32:32 AM UTC-5, Alan Grayson wrote:
>>>
>>>
>>>
>>> On Friday, October 4, 2019 at 4:50:12 AM UTC-6, Lawrence Crowell wrote:
>>>>
>>>> On Friday, October 4, 2019 at 5:34:42 AM UTC-5, Alan Grayson wrote:
>>>>>
>>>>> On Friday, October 4, 2019 at 3:31:31 AM UTC-6, Lawrence Crowell wrote:
>>>>>>
>>>>>> On Thursday, October 3, 2019 at 8:13:22 PM UTC-5, Alan Grayson wrote:
>>>>>>>
>>>>>>> On Thursday, October 3, 2019 at 7:05:12 PM UTC-6, Lawrence Crowell 
>>>>>>> wrote:
>>>>>>>>
>>>>>>>> On Thursday, October 3, 2019 at 8:01:49 PM UTC-5, Lawrence Crowell 
>>>>>>>> wrote:
>>>>>>>>>
>>>>>>>>> On Thursday, October 3, 2019 at 6:59:35 PM UTC-5, Bruce wrote:
>>>>>>>>>>
>>>>>>>>>> On Fri, Oct 4, 2019 at 9:54 AM Alan Grayson <[email protected]> 
>>>>>>>>>> wrote:
>>>>>>>>>>
>>>>>>>>>>>
>>>>>>>>>>> ISTM, that the argument the universe was NOT in thermo 
>>>>>>>>>>> equilibrium just before inflation is alleged to have begun, is 
>>>>>>>>>>> extremely 
>>>>>>>>>>> WEAK. Thus, it's illogical to claim that inflation "smooths out" 
>>>>>>>>>>> the 
>>>>>>>>>>> alleged NON thermo equiiibrium just before inflation begun. AG 
>>>>>>>>>>>
>>>>>>>>>>
>>>>>>>>>> That is essentially what I said. Lawrence is just replacing one 
>>>>>>>>>> set of unknown initial conditions with another, equally unjustified, 
>>>>>>>>>> set.
>>>>>>>>>>
>>>>>>>>>> Bruce
>>>>>>>>>>
>>>>>>>>>
>>>>>>>> In below & means δ. I forgot to replace them.
>>>>>>>>
>>>>>>>> LC
>>>>>>>>  
>>>>>>>>
>>>>>>>>>
>>>>>>>>> The entropy is S = A/4ℓ_p^2 +  quantum corrections, where these 
>>>>>>>>> corrections are ~ (&S/&h^a)k^a. Here h^a is tangent to the horizon 
>>>>>>>>> and k^a 
>>>>>>>>> is normal. This condition coincident on a null surface can appear on 
>>>>>>>>> a 
>>>>>>>>> quantum extremal surface with null tangent g^s so that (&S/&h^a)k^a ≥ 
>>>>>>>>> (&S/&g^a)k^a by subadditivity. However, this surface occurs inside 
>>>>>>>>> the 
>>>>>>>>> cosmological horizon. This means there is no equilibriium. 
>>>>>>>>> Equilibrium is 
>>>>>>>>> only approximated by stretching the horizon out to enormous distance 
>>>>>>>>> after 
>>>>>>>>> the spatial surface has inflated. 
>>>>>>>>>
>>>>>>>>> It is the case that inflation does not tell us the whole story 
>>>>>>>>> prior to inflation. So one can say there are equally unknown initial 
>>>>>>>>> conditions. However, the details of those are less important as the 
>>>>>>>>> spatial 
>>>>>>>>> manifold is stretched out. That means inflation does provide at least 
>>>>>>>>> a 
>>>>>>>>> working system. 
>>>>>>>>>
>>>>>>>>> LC
>>>>>>>>>
>>>>>>>>
>>>>>>> Assuming the universe was incredibly tiny prior to inflation, and 
>>>>>>> was therefore causally connected, isn't it reasonable to assume that it 
>>>>>>> had 
>>>>>>> reached thermo equilibrium *prior* to the onset of inflation? AG 
>>>>>>>
>>>>>>
>>>>>> Thermal equilibrium is not possible with quantum fields in curved 
>>>>>> spacetiome, nor is is likely in quantum gravity. The reason is not too 
>>>>>> hard 
>>>>>> to see. Suppose you have a black hole in a thermal background with the 
>>>>>> same 
>>>>>> temperature as its horizon T ~ 1/8M. The black hole has an 
>>>>>> equiprobability 
>>>>>> of absorbing or emitting a photon with energy δM The temperature then 
>>>>>> adjusts as T - δT ~ 1/8(M + δM) or T + δT ~ 1/8(M - δM) and is shifted 
>>>>>> away 
>>>>>> from thermal equality. This will then enhance the probability the black 
>>>>>> hole either then grows by absorbing more photons or by emitting them. 
>>>>>> There 
>>>>>> is no thermal equilibrium. Quantum gravitation is likely the same, for 
>>>>>> the 
>>>>>> effective specific heat of event horizons is negative. What I wrote 
>>>>>> above 
>>>>>> is in effect a more general form of this.
>>>>>>
>>>>>> Now a gemish of particles or a gas can be in thermal equilibrium in 
>>>>>> spacetime. 
>>>>>>
>>>>>
>>>>> *Doesn't this characterize the universe before inflation began? If 
>>>>> not, then what? AG*
>>>>>
>>>>
>>>> No, the large plasma of particles was generated in the post 
>>>> inflationary period with reheating or the collapse of the vacuum or 
>>>> inflaton.
>>>>
>>>> LC
>>>>
>>>
>>> If not a plasma of particles before inflation, then what was it -- a 
>>> soup of photons, or what? Also, although I really don't know much about 
>>> BH's, your analysis above depends on a boundary between the BH and what's 
>>> beyond it. In the pre-inflation universe there was no internal boundary 
>>> within the universe, so I don't see the relevance of the BH analogy. AG 
>>>
>>
>> I will write it one more time. Particles and radiation emerged in the 
>> observable universe, or this pocket world, with the collapse of the vacuum 
>> energy or inflaton by the mass-gap. The drop in vacuum energy produced the 
>> matter and radiation around us.
>>
>> LC
>>
>
> OK; no particles or radiation prior to the onseet of inflation. But 
> supposing your model is correct, given the incredibly small size of the 
> universe as inflation proceeded, wouldn't those particles and radiation, 
> once created, have been in thermal equilibrium throughout, supporting my 
> model that inflation preserves the thermal equilibrium of the very early 
> universe, but doesn't create it (as measured in the CMBR)? I agree with 
> Clark (and you?) about flatness and monopoles, but I think he didn't 
> understand my reason for thinking the very early universe was in thermal 
> equilbrium, and that this state wasn't created, but *preserved* by 
> inflation. AG 
>

They came to equilibrium, and what thermal fluctuations that deviated away 
from equilibrium were "ironed out" by inflation. The current state of the 
universe is such that it emerged from a much lower state of entropy than 
what we would otherwise think. This state of low entropy was available to a 
causal region that inflated out, and what fluctuations existed were 
stretched out and reduced in relative magnitude.

I fail to see why so many people have trouble with this. It is not a final 
answer, for that will require not only quantum gravitation, but a theory of 
quantum gravitation that is worked into a fair measure of maturity. 
However, inflation does push the barrier of ignorance back a fair degree.

LC
 

>  
>>
>>>  
>>>>
>>>>>  
>>>>>
>>>>>> That was what was set up with inflation. The whole process of the 
>>>>>> early expanding universe is about there being episodes of approximate 
>>>>>> thermal equilibrium of particles, such as during the quark-gluon plasma 
>>>>>> phase, electroweak period, the QED equilibrium of electrons and photon 
>>>>>> or 
>>>>>> the plasma phase that ended by producing the CMB. 
>>>>>>
>>>>>> To think about physics one has to do a sort of Buddhist middle way. 
>>>>>> It is not good to either be too liberal or given to extreme 
>>>>>> speculations, 
>>>>>> but it is also not good to be overly conservative. 
>>>>>>
>>>>>> LC 
>>>>>>
>>>>>

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