On Wednesday, May 23, 2018 at 11:20:48 PM UTC, Brent wrote:
>
>
>
> On 5/23/2018 3:53 PM, [email protected] <javascript:> wrote:
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>
>
> On Wednesday, May 23, 2018 at 5:54:29 PM UTC, Brent wrote: 
>>
>>
>>
>> On 5/22/2018 11:53 PM, [email protected] wrote:
>>
>>
>>
>> On Wednesday, May 23, 2018 at 4:44:30 AM UTC, Brent wrote: 
>>>
>>>
>>>
>>> On 5/22/2018 9:41 PM, [email protected] wrote:
>>>
>>>
>>>
>>> On Wednesday, May 23, 2018 at 4:05:58 AM UTC, Brent wrote: 
>>>>
>>>>
>>>>
>>>> On 5/22/2018 8:29 PM, [email protected] wrote:
>>>>
>>>>
>>>>
>>>> On Wednesday, May 23, 2018 at 2:24:07 AM UTC, Bruce wrote: 
>>>>>
>>>>> From: <[email protected]>
>>>>>
>>>>>
>>>>> On Wednesday, May 23, 2018 at 1:45:39 AM UTC, Brent wrote: 
>>>>>>
>>>>>>
>>>>>>
>>>>>> On 5/22/2018 5:59 PM, [email protected] wrote:
>>>>>>
>>>>>>
>>>>>>
>>>>>> On Wednesday, May 23, 2018 at 12:44:06 AM UTC, Brent wrote: 
>>>>>>>
>>>>>>>
>>>>>>>
>>>>>>> On 5/22/2018 3:46 PM, [email protected] wrote:
>>>>>>>
>>>>>>>
>>>>>>>
>>>>>>> On Tuesday, May 22, 2018 at 10:41:11 PM UTC, [email protected] 
>>>>>>> wrote: 
>>>>>>>>
>>>>>>>>
>>>>>>>>
>>>>>>> I did, but you're avoiding the key point; if the theory is on the 
>>>>>>> right track, and I think it is, quantum measurements are irreversible 
>>>>>>> FAPP. 
>>>>>>> The superposition is converted into mixed states, no interference, and 
>>>>>>> no 
>>>>>>> need for the MWI. 
>>>>>>>
>>>>>>>
>>>>>>> You're still not paying attention to the problem.  First, the 
>>>>>>> superposition is never converted into mixed states.  It 
>>>>>>> *approximates*, FAPP, a mixed state* in some pointer* basis (and 
>>>>>>> not in others).  Second, even when you trace over the environmental 
>>>>>>> terms 
>>>>>>> to make the cross terms practically zero (a mathematical, not physical, 
>>>>>>> process) you are left with different outcomes with different 
>>>>>>> probabilities.  CI then just says one of them happens.  But when did it 
>>>>>>> happen?...when you did the trace operation on the density matrix?
>>>>>>>
>>>>>>
>>>>>> I think the main takeaway from decoherence is that information isn't 
>>>>>> lost to other worlds, but to the environment in THIS world. 
>>>>>>
>>>>>>
>>>>>> But that ignores part of the story.  The information that is lost to 
>>>>>> the environment is different depending on what the result is.   So if by 
>>>>>> some magic you could reverse your world after seeing the result you 
>>>>>> couldn't get back to the initial state because you could not also 
>>>>>> reverse 
>>>>>> the "other worlds".
>>>>>>
>>>>>
>>>>> What "other worlds"? If they don't exist, why should I be concerned 
>>>>> about them? AG
>>>>>
>>>>>
>>>>> I think you are ignoring the facts of the mathematics of unitary 
>>>>> evolution of the wave function. Under unitary evolution the wave function 
>>>>> branches, one branch or each element of the superposition, which is, one 
>>>>> branch for each possible experimental result. These branches are in the 
>>>>> mathematics. Now you can take all branches as really existing every much 
>>>>> as 
>>>>> the observed result exists -- that is the MWI position. Or you can throw 
>>>>> them away as not representing your experimental result -- which is the 
>>>>> collapse position. But in both cases, the evolution of the wave function 
>>>>> shows that there is information in each mathematical branch. If you 
>>>>> discard 
>>>>> the branches (collapse) you throw this information away: if you retain 
>>>>> the 
>>>>> branches as other worlds, the information becomes inaccessible by 
>>>>> decoherence and partial tracing.
>>>>>
>>>>> The situation is the same in either approach. Brent and I are not 
>>>>> being inconsistent, devious, or otherwise tricky by referring to both MWI 
>>>>> and CI approaches -- we are just recognizing the actual mathematics of 
>>>>> quantum mechanics. The mathematics has to be interpreted, and different 
>>>>> interpretations are available for the way in which the information in 
>>>>> other 
>>>>> branches is treated.
>>>>>
>>>>> Bruce
>>>>>
>>>>
>>>> Consider this interpretation of the wf, which for simplicity I consider 
>>>> as a superposition of two eigenfunctions, and based on the probability 
>>>> amplitudes represents a 50% probability of each outcome at some point in 
>>>> time. Since the measurement hasn't occurred, where does this information 
>>>> reside? Presumably it all resides in THIS world. As time evolves the 
>>>> probability distribution changes, say to 75-25, and later to 90-10, and so 
>>>> on. All of this information resides in this world since without a 
>>>> measurement occurring, there are no other worlds, and no collapse. Suppose 
>>>> at some point in time, the values changed to 100-0, Isn't 100-0 as good as 
>>>> other pair if they sum to zero? And why would anyone think another world 
>>>> comes into existence because one of the values evolved to 0? I will now 
>>>> define, in answer to one of Brent's questions, when the measurement 
>>>> occurs. 
>>>> I assert it occurs when one of the pair of values equals 0, All throughout 
>>>> all information was in this world. Why would another world come into 
>>>> existence if one of the values happened to be 0? AG
>>>>
>>>>
>>>> First, in the cases of interest there is no mechanism for going from 
>>>> 50/50 to 100/0 because it goes 0/100 as well, and it's random.  You may 
>>>> hypothesize there is such process, but that's equivalent to assuming a 
>>>> hidden variable.  And then Aspect's experiments show such a hidden 
>>>> variable 
>>>> transmits influence faster than light...which then cascades into problems 
>>>> with special and general relativity and quantum field theory and so on...
>>>>
>>>> Brent
>>>>
>>>
>>> I was assuming the wf evolves to different probabilities via the SWE. 
>>> Nothing wrong with going to 0/100 because that just means the other 
>>> eigenvalue became the final state. AG 
>>>
>>>
>>> That's why I wrote "in cases of interest".  If it evolves to 0/100 via 
>>> the SWE no problem...no interest either.
>>>
>>
>> Why no interest? Haven't I described the case of a system evolving 
>> according to the SWE, then a measurement occurring, and throughout all the 
>> information is residing in THIS world. Why would information be lost to 
>> some other world simply because one value of the pair of probabilities 
>> equals 0? AG
>>
>>
>> It wouldn't if the SE caused it to evolve to 0.  But in the cases of 
>> interest the SE causes the reduced density matrix to evolve to non-zero 
>> diagonal elements and the cross terms to be zero FAPP (but not exactly) so 
>> that it approximates a mixed state density matrix.  Then we say each 
>> diagonal element is the probability amplitude of a "world" as if the off 
>> diagonal terms were exactly zero.
>>
>
> Do you have some good links which explains this? AG
>
>
> https://arxiv.org/pdf/quant-ph/0312059.pdf
>
> Also, I think these other "worlds" are just inaccessible, disjointed 
> subspaces corresponding to the values which are NOT measured in this world, 
> and this concept has been distorted for (and by) the hoi polloi to mean 
> actual, full blown, copies of this world, including copies of the original 
> observer, his/her memories, and so forth. Is this your understanding as 
> well; that these full blown copies of this world and its observer do NOT 
> exist? AG
>
>
> In the MWI interpretation there is no reason to preference one over the 
> other with the honorific of "exists".  They are just projective subspaces 
> that are essentially (FAPP) orthogonal to one another. 
>

I can buy that, although tentatively, with difficulty, until I see the 
mathematics which demonstrates it. AG
 

> Each one includes copies of the system, the environment, and the 
> observer(s) which is necessary so that it constitute a classical "world" in 
> which everyone agrees on the result.
>

This I absolutely CANNOT buy, as I have explained numerous times. Cannot 
decoherence and the MWI have descriptive value without all of this COPYING 
being assumed, which I find outlandish? Would it be fatal to any of these 
concepts to affirm that the entanglements which occur in these subspaces 
are equivalent to measurements in these subspaces? AG

>
> Brent
>

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