On Wed, Oct 9, 2019 at 11:36 AM 'Brent Meeker' via Everything List <
[email protected]> wrote:

> On 10/8/2019 5:03 PM, Bruce Kellett wrote:
>
> On Wed, Oct 9, 2019 at 10:49 AM 'Brent Meeker' via Everything List <
> [email protected]> wrote:
>
>> On 10/8/2019 4:21 PM, Bruce Kellett wrote:
>>
>> On Wed, Oct 9, 2019 at 9:53 AM 'Brent Meeker' via Everything List <
>> [email protected]> wrote:
>>
>>
>>> What additional assumptions do you mean?
>>>
>>
>> What assumptions does he have to make to get a probability
>> interpretation? Probability is not an evident property of the SE. Like many
>> approaches to probability in Everett, he has to assume decoherence to
>> distinguishable branches to get anywhere. But that relies on using the Born
>> rule to justify ignoring branches with low amplitude
>>
>> The low amplitude branches aren't ignored.  Do you mean cross-terms in
>> the density matrix?
>>
>
> Explain to me how these are functionally different from low amplitude
> branches.
>
>
> The branches are projections of the universal Hilbert ray onto
> (approximately) orthogonal subspaces corresponding to the preferred basis.
> Cross terms are what make them approximate.  The cross-terms supposedly go
> to zero when you compute the reduced density matrix, but the diagonal terms
> don't go to zero...they measure the probability of the branches, including
> branches with low probability.
>

It seems to me that that is what I said.


> -- the notorious "trace over environmental degrees of freedom". Sean's
>> "self-locating uncertainty" is not well-defined.
>>
>>
>> I tend to agree with you there.  But if you assume that the human brain
>> is a classical information processor of limited capacity I think you could
>> get there.
>>
>
> Only at the price of re-introducing the human observer into your
> exposition of QM. I thought that was the cardinal sin of the CI, and here
> Sean is bringing it back into Everett!!!!
>
>
> Well, if you're going to explain why we experience a classical world,
> you're going to have to say something about experience.  To say it's
> information processing in the brain sounds pretty good to me.
>

But that is what he needs in order to introduce probabilities -- and that
is just as circular as the Deutsch-Wallace use of decision theory -- both
need observers to have a notion of probability.


> In the lecture he hints that the observer is uncertain about the fate of
>> the cat until he opens the box -- until then he is uncertain of which
>> branch he is on. But given the timescale of decoherence, he has branched
>> within 10^{-20} sec, so the is no longer any "self-locating uncertainty" --
>> he is definitely on one branch or the other, he just doesn't know which.
>> And that is just classical probability due to lack of knowledge -- nothing
>> quantum about it. In another interview, he does suggest that the
>> "self-locating uncertainty" lasts only until decoherence reaches the
>> observer, at which time copies become entangled within each branch. Now if
>> you can think relevant thoughts in 10^{-20} sec, then his argument might
>> make some sense. But it fails to convince.....
>>
>>
>> So you're faulting him for not calling 1e-20sec zero?
>>
>
> No. I am not faulting him for not calling it zero. I am faulting him for
> calling something that is uncertain in any quantum sense for 10^{-20} sec
> significant for the interpretation of probabilities.
>
> But it's relevant to showing MWI is consistent with the experimenter not
> knowing which "world" he is in. He might not look at the data for a long
> time.
>

Exactly. So his "uncertainty" is purely classical. That is not an
explanation of quantum probabilities. Remember, the Everettian promise is
that the concept of "an observer" is irrelevant for understanding the
theory -- it is all in the SWE. The theory provides its own
explanation......

Bruce

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