You are still assuming that each measurement results in a discrete split
with exactly one observer per branch, which is an interpretation, not a
derivation. Nothing in the Schrödinger equation forces branches to be
discrete rather than continuously superposed structures with relative
measure. Your reasoning assumes what it wants to prove: that branching is a
countable process rather than a differentiation of an already superposed
structure.

Publish it, what are you afraid of? Being proved wrong?

Quentin

Le mer. 26 févr. 2025, 11:04, Bruce Kellett <[email protected]> a
écrit :

> On Wed, Feb 26, 2025 at 7:08 PM Quentin Anciaux <[email protected]>
> wrote:
>
>> Le mer. 26 févr. 2025, 01:53, Brent Meeker <[email protected]> a
>> écrit :
>>
>>> On 2/25/2025 5:09 PM, Russell Standish wrote:
>>>
>>> On Wed, Feb 26, 2025 at 11:01:11AM +1100, Bruce Kellett wrote:
>>>
>>>     On 2/24/2025 6:09 PM, Quentin Anciaux wrote:
>>>
>>>         Your claim that "one observer per branch" follows directly from 
>>> unitary
>>>         evolution is an assumption, not a derivation.
>>>
>>>
>>> No, it is a straightforward derivation from the formalism. If you don't
>>> understand that, it is just further confirmation of the fact that you
>>> understand very little about quantum mechanics.
>>>
>>> Not at all - it is an assumption you're making, and the nub of the entire
>>> argument between you and Quentin.
>>>
>>> Do you understand Quentin's theory?  ISTM it's just "Observer counting"
>>> where the counts instantiate the Born rule ex hypothesi.  It's branch
>>> counting by another name.
>>>
>>> Brent
>>>
>>
>> Brent,
>>
>> You’re still misrepresenting the argument. It’s not branch counting under
>> another name, it’s about how measure determines observer frequencies. The
>> issue is whether the number of observer instances scales with amplitude
>> squared, not whether we simply count branches. If all branches were
>> weighted equally, MWI would have been dead on arrival, because it wouldn’t
>> match experiments.
>>
>> The claim that “one observer per branch” is a direct consequence of
>> unitary evolution is just an assumption, it’s not something derived from
>> the Schrödinger equation.
>>
>
> It is derived from that, or the Schrodinger equation enhanced with unitary
> evolution and the linearity of Hilbert space.
>
> Since you clearly don't get it. Let me spell it out in baby steps.
>
> We start from the wave function for some system, say |psi>. This is the
> expanded in some basis like |psi> = a|0> + b|1>, where I have taken a two
> dimensional space for clarity and convenience, although the argument is
> easily expanded to an arbitrary number of independent basis states.
>
> We then measure this state (or subject it to some interaction).
> |psi>|O>|E> where |O> is an observer, and |E> is the environment which can
> include anything else that is relevant. Linear unitary evolution then
> entangles both the observer and the environment with the object state:
>
>          |psi>|O>|E> = (a|0> + b|1>)|O>|E> --> a|O sees zero>|E records
> zero>|0> + b|O sees one>|E records one>|1>,
>
> One can readily see that there is one, and only one, copy of the observer
> for each branch. Decoherence renders these branches approximately
> orthogonal, and leads to the notion of independent worlds. The argument
> can, of course, be readily generalized to a state with any number of basis
> vectors. In no case, do we get more than one copy of the observer on any
> branch, and there are no branches without a copy of the observer.
>
> All of this is just elementary linear unitary evolution, taught in general
> quantum mechanics courses. If you want to deny this, you have to go to some
> other theory which is incompatible with quantum mechanics.
>
> Bruce
>
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