Brent,

That assumes a strict one-to-one mapping between observers and branches,
which is exactly what’s in question. If the wavefunction remains a
superposition of infinite branches, then what we call a "branch" is just a
coarse-grained partition, not a fundamental unit.

If we allow infinite superposition, partitioning the multiverse by
amplitude isn’t the same as naive branch counting. It’s closer to a
measure-based weighting, where high-amplitude outcomes have exponentially
more observer instances—not more branches, but more weight within the
structure.

If you assume one observer per branch, you assume what you want to prove:
that measure plays no role. But if measure defines how often an observer
finds themselves in a given state, it naturally leads to the Born rule
without naive branch counting.

Quentin

Le jeu. 20 févr. 2025, 00:43, Brent Meeker <[email protected]> a écrit :

>
>
> On 2/19/2025 12:20 AM, Quentin Anciaux wrote:
>
> Brent,
>
> Yes, and that’s exactly the problem—Gleason’s theorem doesn’t apply to
> two-dimensional Hilbert spaces, which means it doesn’t universally derive
> the Born rule. So if MWI fails for not deriving the Born rule, then
> standard QM faces the same issue unless you introduce additional
> postulates.
>
> Branch counting doesn’t work, but my example isn’t branch counting—it’s
> asymmetric duplication, where observer distribution follows measure,
>
> Observer distribution is only one observer per branch; the observers can't
> see each other.  So N observers implies N branches.  It's mathematically
> equivalent to branch counting.
>
> Brent
>
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