On Wednesday, April 20, 2022 at 5:21:47 PM UTC-6 Alan Grayson wrote:

>
>
> On Friday, April 15, 2022 at 12:41:03 PM UTC-6 [email protected] wrote:
>
>>
>>
>> On 4/14/2022 2:00 PM, George Kahrimanis wrote:
>>
>> On Wednesday, April 13, 2022 at 8:55:48 PM UTC+3 [email protected] 
>> (Brent) wrote:
>>
>> Decoherence has gone part way in solving the when/where/what basis 
>>> questions, but only part way.
>>>
>>
>> As I wrote at the end of my first reply to your message, I share your 
>> concern about decoherence but I see the glass as half-full; that is, with a 
>> little more subtlety I hope that the matter can be formulated in clear 
>> terms.
>>
>> Surely collapse is easier to handle as a general concept (except, on the 
>> other hand, that it requires new dynamics). I forgot to mention that *my 
>> argument for deriving the Born Rule works with collapse, too* -- so it 
>> is an alternative to Gleason's theorem.
>>
>> Here I define colapse as an irreversible process, violating unitarity of 
>> course, and I keep it separate from randomisation. The latter means that 
>> each outcome is somehow randomised -- an assumption we can do without.
>>
>> *Collapse can also be described in a many-world formulation!* It differs 
>> from the no-collapse MWI only in being irreversible. 
>>
>>
>> If you can throw away low probability branches, what's to stop you from 
>> throwing away all but one?  You've already broken unitary evolution.  If 
>> you read Hardy's axiomatization of QM you see that the difference between 
>> QM and classical mechanics turns on a single word in Axiom 5 Continuity: 
>> There exists a *continuous *reversible transformation on a system 
>> between any two pure states of that system.
>>
>> My argument in outline is
>> 1. assessment that MWI-with-collapse is workable;
>> 2. therefore, outcomes of small enough measure can be neglected in 
>> practice;
>>
>>
>> Yes, I've wondered if a smallest non-zero probability could be defined 
>> consistent with the data.
>>
>> 3. now Everett's argument can proceed, concluding that the Born Rule is a 
>> practically safe assumption (to put it briefly).
>>
>> So I have replaced two assumptions of Gleason's theorem, randomisation 
>> and non-contextuality, by the assessment of workability only.
>>
>> If you don't feel comfortable yet with formulating collapse in a 
>> many-world setting, let us also assume randomisation (God plays dice), for 
>> the sake of the argument, in a single-world formulation. That is, we ASSUME 
>> the existence of probability; then the previous argument just guarantees 
>> that this probability follows the Born Rule.
>>
>>
>> Assume?  Randomness is well motivated by evidence.  And it's more random 
>> than just not knowing some inherent variable, because in the EPR experiment 
>> a randomized hidden variable can on explain the QM result if it's non-local.
>>
>
>>
>>
>> Of course I favour the first version of the argument, using the 
>> many-world formulation of collapse, to avoid the "God plays dice" nightmare.
>>
>>
>> Why this fear of true randomness?  We have all kinds of classical 
>> randomness we just attributed to "historical accident".  Would it really 
>> make any difference it were due to inherent quantum randomness?  Albrect 
>> and Phillips have made an argument that there is quantum randomness even 
>> nominally classical dynamics. https://arxiv.org/abs/1212.0953v3
>>
>
> The authors regard quantum fluctuations as fundamental. How are they 
> defined? AG
>
I think I get it. Whereas before QM we could attribute single, unpredicted 
outcomes to ignorance of initial conditions, and but with QM our 
understanding is augmented; now we can attribute it to ... nothing? AG

>
>> Brent
>>
>>
>> Thanks for the comments so far, because they stirred my thinking and 
>> motivated fresh ideas, some of which I hope will prove helpful and worth 
>> discussing, if and when they mature.
>>
>> George K.
>>
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