> On 17 Feb 2020, at 23:46, 'Brent Meeker' via Everything List 
> <[email protected]> wrote:
> 
> 
> 
> On 2/17/2020 2:11 AM, Bruce Kellett wrote:
>> On Mon, Feb 17, 2020 at 6:04 PM 'Brent Meeker' via Everything List 
>> <[email protected] <mailto:[email protected]>> 
>> wrote:
>> On 2/16/2020 9:48 PM, Bruce Kellett wrote:
>>> On Mon, Feb 17, 2020 at 4:13 PM 'Brent Meeker' via Everything List 
>>> <[email protected] 
>>> <mailto:[email protected]>> wrote:
>>> 
>>> But exactly the same reasoning applies for any given true value of p.  
>>> There will be different estimates by different experimenters and they can't 
>>> all be right.  Each will infer that any proportion other than the one he 
>>> observed will have zero measure in the limit N->oo.
>>> 
>>> Exactly right. That is what my example of spin measurements on an ensemble 
>>> of equally prepared spin states comes into play. If all 2^N bit strings are 
>>> realized for one orientation of the S-G magnet, then exactly the same 2^N 
>>> bit strings are realized for every other orientation. 
>> 
>> ?? Suppose the ensemble is equally prepared in spin-up.  What does it mean 
>> to say all 2^N bit strings are realized for the S-G oriented left/right?  We 
>> may expect they will be for any number of trials >>N.  But certainly  not 
>> for the S-G oriented up/down.
>> 
>> I think we are beginning to argue at cross-purposes, and I may not have 
>> understood you correctly. Let me try to restate the position clearly, and 
>> see if you can agree.
>> 
>> Take a spin-half state, and prepare a linear combination in the x-basis:
>> 
>>        |psi> = (alpha*|x-spin up> + beta*|x-spin down>),
>> 
>> where we assume that neither alpha nor beta is equal to zero. We can now 
>> measure this state in the x-direction and assume Everett, so that every 
>> result is obtained in a separate branch on every trial. Coding these results 
>> as zero and one, a run of N experiments will give 2^N binary strings of 
>> results, consisting of the set of all 2^N binary strings of length N. Now 
>> rotate the S-G magnet from the x-direction by, say, 10 degrees. Your results 
>> are again the set of all binary strings of length N. Similarly for any other 
>> angle (except those for which alpha or beta rotates to zero). Since the set 
>> of results is the same in all cases, even though rotation of the S-G magnet 
>> is equivalent to changing alpha and beta in the superposition, the 
>> individual sets of results must be independent of alpha and beta. However, 
>> the Born rule states that the probabilities depend on |alpha|^2 and |beta|^. 
>> But we have seen that the many-worlds data are actually independent of alpha 
>> and beta. The Born rule for probabilities is thus disconfirmed in this 
>> Everettian case.
>> 
>> That is the crux of what I am trying to get across -- Everettian QM is 
>> disconfirmed by experiment, since experiments show results that depend on 
>> the coefficients alpha and beta, in accordance with the Born Rule. There are 
>> other points that I have been making, but let's get this straight first.
> 
> Yes, I agree with that.  It's another way of expressing my objection that 
> while alpha=0.5 produces a split into two worlds, alpha= 0.499 produces a 
> split into a thousand worlds.
> 
> But proponents of MWI like Sean Carroll and Bruno, essentially assume there 
> are already (infinitely?)

Yes, infinitely, as your own example of 0.499 already suggest. Recently I have 
found reason that it could even be a *very* large cardinal (I really don’t 
know, but some axioms in set theory do provide light on the measure problem,  
It is very technical alas.

Bruno




> many branches which, prior to the measurement, are identical at the 
> macroscopic level, but which get projected (split) onto orthogonal subspaces 
> by a measurement.  
> 
> Brent
> 
>> 
>> Bruce
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