Bruce,

I’ve already provided multiple counterexamples, but you keep repeating the
same assertions as if that’s a substitute for addressing them. If you’re so
convinced of your "proof," publish it instead of endlessly posturing here.
Otherwise, this is just noise.

Quentin

Le mer. 26 févr. 2025, 22:08, Bruce Kellett <[email protected]> a
écrit :

> On Wed, Feb 26, 2025 at 10:26 PM Quentin Anciaux <[email protected]>
> wrote:
>
>> 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.
>>
>
> I find it interesting that you haven't even attempted to answer the
> detailed argument that I made (below). That, to me, suggests that you do
> not have any coherent response to offer. So you just repeat your normal
> smoke-and-mirrors trick and hope that I will be diverted away from the main
> points. I think you need to up your game if you want to make any progress
> here.
>
> Bruce
>
>
>> 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:
>>>
>>>>
>>>> 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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