On Thu, Aug 28, 2025 at 3:52 PM Jesse Mazer <[email protected]> wrote:

> On Thu, Aug 28, 2025 at 12:49 AM Bruce Kellett <[email protected]>
> wrote:
>
>> On Thu, Aug 28, 2025 at 2:30 PM Brent Meeker <[email protected]>
>> wrote:
>>
>>> On 8/27/2025 5:07 PM, Bruce Kellett wrote:
>>>
>>> On Thu, Aug 28, 2025 at 5:16 AM Brent Meeker <[email protected]>
>>> wrote:
>>>
>>>> I think some specificity would help this debate.  Suppose N=6, so there
>>>> are 64 different sequences in 64 different worlds.  The number of observers
>>>> is irrelevants; we can suppose the results are recorded mechanically in
>>>> each world.  Further suppose that a=b so there is no question of whether
>>>> amplitudes are being respected.  Then in one of the worlds we have 011000.
>>>> Per the Born rule its probability is 0.2344.  In MWI it is 1/64=0.0156.
>>>> The difference arises because the observers applying the Born rule looks at
>>>> it as an instance of 2 out of 6 successes.
>>>>
>>>
>>> The trouble with this is that you are treating this as an instance of
>>> Bernoulli trials with probability p= 0.5. When every outcome occurs with
>>> every trial we no longer have a Binomial distribution The Binomial
>>> distribution assumes that you have x successes out of N trials. In the
>>> Everettian case you have one success on every trial.
>>>
>>> So your probability above for 2 successes applies to Bernoulli trials
>>> with one as the 'success'. The thing is that the probability of getting a
>>> zero is also 1/2, so we also have four successes out of six trials in your
>>> example. The Binomial probability for this result is also 0.2344. Actually,
>>> if we regard this experiment as a test of the Born rule, we have four zeros
>>> in 6 trials, which gives an estimate of the probability as 4/6 = 0.667, or
>>> as two ones in 6 trials which gives an estimate of the probability as 2/6 =
>>> 0.333, neither estimate is equivalent to |a|^2 = 0.5. The difference
>>> becomes more pronounced as N increases. The problem with your analysis is
>>> that you are assuming a binomial distribution. and we do not have any such
>>> distribution.
>>>
>>> That's how an experimenter will compute the probability of 2 successes
>>> in 6 trials given p=0.5.   Yes, the probability estimate is 0.33 given 2 in
>>> 6.  The probability of the result given p is not generally the same as the
>>> estimate of p given the result.  The former is binomial distributed.  The
>>> estimates of p aren't part of a distribution since they don't add up to 1.
>>>
>>
>> You are still assuming that the results follow a binomial distribution.
>> This is not the case. As I said, in the Everett situation, when every
>> outcome is realized in every trial, you have one success in every trial,
>> and the resulting distribution is not binomial. The normal approximation
>> for large N, as Jesse seems to assume, simply does not hold, since the
>> distribution is not binomial.
>>
>
> I don't assume anything myself, I point to some sources by physicists
> below indicating there is a mathematical derivation of the fact that if
> physical records ('pointer states') of a series of N trials are kept, and
> you define a measurement operator that only tells you the fraction of those
> recorded trials with some result, then one can show that the deterministic
> equation of wavefunction evolution (without collapse assumption/Born rule)
> implies that the quantum state of the records approaches the "correct"
> eigenstate of this measurement operator (the one that matches what would be
> predicted using the Born rule) in the limit as N approaches infinity.
>
> https://books.google.com/books?id=_HgF3wfADJIC&lpg=PP1&pg=PA238
>
> https://www.academia.edu/6975159/Quantum_dispositions_and_the_notion_of_measurement
>



It is not clear how this applies to the case under discussion. Could you be
more specific?

Bruce

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