On Wednesday, January 27, 2021 at 3:56:50 AM UTC-7 Quentin Anciaux wrote:

>
>
> Le mer. 27 janv. 2021 à 11:54, Alan Grayson <[email protected]> a 
> écrit :
>
>>
>>
>> On Tuesday, January 12, 2021 at 10:19:59 PM UTC-7 Pierz wrote:
>>
>>>
>>>
>>> On Monday, January 4, 2021 at 12:09:06 PM UTC+11 [email protected] 
>>> wrote:
>>>
>>>> On Sunday, January 3, 2021 at 3:56:51 PM UTC-7 [email protected] 
>>>> wrote:
>>>>
>>>>> On Sun, Jan 3, 2021 at 5:21 PM Alan Grayson <[email protected]> 
>>>>> wrote:
>>>>>
>>>>> *> The MWI doesn't guarantee that these subsequent measurements, for 
>>>>>> subsequent horse races say, are occurring in the SAME OTHER worlds as 
>>>>>> trials progress, to get ensembles in those OTHER worlds. *
>>>>>
>>>>>  
>>>>> I don't know what you mean by "SAME OTHER worlds", the same as what? 
>>>>> In one world Alan Grayson remembers having seen the electron go left, in 
>>>>> another world Alan Grayson remembers having seen the electron go right, 
>>>>> other than that the two worlds are absolutely identical, so which one was 
>>>>> the "SAME OTHER world"?
>>>>>
>>>>> > You seem to avoid the fact that no where does the MWI guarantee 
>>>>>> [...]
>>>>>
>>>>>
>>>>> Quantum mechanics is not in the guarantee business, it deals with 
>>>>> probability.  
>>>>>
>>>>> *> I don't think you understand my point, which isn't complicated. *
>>>>>
>>>>>
>>>>> Yes, your point is very simple indeed, but the word simple can have 2
>>>>>  meanings, one of them is complementary and the other not so much.  
>>>>>
>>>>
>>>> In first trial, the MWI postulates other worlds comes into existence. 
>>>> Same other worlds in second trial? Same other worlds in third trial, etc? 
>>>> Where does the MWI assert these other worlds are the SAME other worlds? 
>>>> Unless it does, you only have ONE measurement in each of these worlds. No 
>>>> probability exists in these other worlds since no ensemble of measurements 
>>>> exist in these other world. AG
>>>>
>>>  
>>> You grossly misunderstand MWI. There are no "same other" worlds. The 
>>> worlds that arise at each trial are different in precisely one way and one 
>>> way only: the eigenvalue recorded for the experiment. The different 
>>> eigenvalues will then give rise to a "wave of differentiations" as the 
>>> consequences of that singular difference ramifies, causing the different 
>>> worlds generated by the original experimental difference to multiply. 
>>> "World" really means a unique configuration of the universal wave function, 
>>> so two worlds at different trials can't possibly be the "same world", and 
>>> yes, there is only one measurement in each. 
>>>
>>  
>> *If there is only one measurement in each other world -- which has been 
>> my claim throughout -- how can Born's rule be satisfied in the MWI? AG*
>>
>
> Every world has a past... So if you do n experiments after n trials you 
> have 2^n number of worlds each having a past of n trials.
>

*On the second trial and another splitting, what is the assurance that the 
new other world is the same as that created on the first splitting, so a 
sequence of measurement history exists? AG*

>
>>
>>  
>>
>>> That is precisely the stipulation of MWI. If we have a quantum 
>>> experiment with two eigenvalues 1 and 0, and each is equally likely per the 
>>> Born rule, then the MWI interpretation is that - effectively - two worlds 
>>> are created. You, the experimenter, end up in both, each version knowing 
>>> nothing about the other. So, in the "objective world" (the view from 
>>> outside the whole wave function as it were), no probability is involved. 
>>> But if you repeat this experiment many times, each version of you will 
>>> record an apparently random sequence of 1s and 0s. Your best prediction of 
>>> what happens in the next experiment is that it's a 50/50 toss up between 1 
>>> and 0. Objectively there's no randomness, subjectively it appears that way.
>>>  
>>>
>>>>  
>>>>
>>>>> John K Clark   See my new list at  Extropolis 
>>>>> <https://groups.google.com/g/extropolis>
>>>>>
>>>> -- 
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