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*
>
AGGGGG*G*
>

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.

>
>
>
>
>> 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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