On Sat, Feb 22, 2020 at 11:35 AM 'Brent Meeker' via Everything List <
[email protected]> wrote:

> On 2/21/2020 4:19 PM, Bruce Kellett wrote:
>
> On Sat, Feb 22, 2020 at 11:11 AM smitra <[email protected]> wrote:
>
>> On 16-02-2020 06:34, Bruce Kellett wrote:
>> >
>> > The probabilistic interpretation of QM arose in a single-world,
>> > collapse, model. Attempting to graft probability on to many-worlds is
>> > a failure, as my arguments against Everett show. If the data for any
>> > sequence of trials are independent of the amplitudes, then some ad hoc
>> > probability interpretation of the amplitudes is not going to affect
>> > the data. But the data is what we use to infer that Born rule
>> > probabilities are what we observe. This is a single-world result.
>> >
>> > Bruce
>>
>> It's only a failure when attempting to describe the state in the
>> multiverse in that particular way where you can argue that the
>> amplitudes don't matter. It's not an argument against the multiverse
>> idea, as whether or not you have a large number of copies should not
>> affect the statistical outcome observed in any experiment.
>>
>
> No. And it has not been suggested that it will. But that is just to take a
> single-world approach: statistics work fine in each branch of the
> multiverse (each world), but the concepts of probability and the Born rule
> break down when every result is obtained in experiments because the data
> obtained in each world are independent of the amplitudes of the original
> state.
>
>
> This objection seems to rest on the idea that the set of sequences (across
> all the worlds) cannot be regarded as an ensemble from which one is picked
> by self-location.
>

I am not  sure what this means. The set of all sequences (all branches or
worlds) is just the set of all 2^N possible binary strings, so any set of
results that an individual might obtain is a selection from this set. If
you want to regard this as self-location, then fine, but I don't know what
that gains you.

Otherwise applying probability theory to the ensemble recovers the
> one-world statistics.  Right?
>

In the two-outcome case, any branch of the ensemble is just a one-world set
of Bernoulli trials, so the statistics of that branch correspond to the
binomial distribution with a probability characteristic of the branch.
Different branches will, in general, correspond to different p-values. The
argument against Everett is that this set of binary strings is independent
of the amplitudes of the initial quantum state so there is no room for the
Born rule.

> Of course you can say there really is no ensemble (that is accessible to
> anyone), but that's true of the hypothetical ensembles invoked in
> statistics all the time.
>


I can't really grasp what your objection to the case I have made is. Is it
anything more than that the result goes against your basic intuitions?

Bruce

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