Le ven. 14 févr. 2025, 16:23, Alan Grayson <[email protected]> a
écrit :

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> On Friday, February 14, 2025 at 2:41:44 AM UTC-7 Quentin Anciaux wrote:
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> Le ven. 14 févr. 2025, 10:29, Alan Grayson <[email protected]> a écrit :
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> On Friday, February 14, 2025 at 2:17:37 AM UTC-7 Quentin Anciaux wrote:
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> Le ven. 14 févr. 2025, 10:08, Alan Grayson <[email protected]> a écrit :
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> On Friday, February 14, 2025 at 1:37:20 AM UTC-7 Quentin Anciaux wrote:
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> Le ven. 14 févr. 2025, 06:13, Brent Meeker <[email protected]> a écrit :
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> On 2/13/2025 4:57 AM, John Clark wrote:
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> On Wed, Feb 12, 2025 at 5:41 PM Brent Meeker <[email protected]> wrote:
>
> *>> Schrodinger's Equation is 100% deterministic, so why is it necessary
> to resort to probability at all?*
>
>
>
> > *Because one thing of many possible happens.*
>
>
>
> *Why is that "one" thing special? I can answer that; because it's not
> special, many things happen, everything that is not forbidden happens. You
> have no answer to that question other than "because it is".  *
>
> The only thing special about is that it's the one that happened.  If
> everything not forbidden happens then you're going to need to explain what
> probabilty means.
>
>
> * > I can write an equation for the toss of die that shows that the
> probability of each face is 1/6.  That equation is deterministic.  It
> determines probabilities. And probabilities tell you that some things
> happen and some don't.  Not that every face of the die comes up on every
> throw.*
>
>
>
> *Schrodinger's equation produces a complex-valued wave that evolves in
> time, the square of the absolute value of the amplitude of that wave
> determines probabilities. You just take the Born Rule as a given because
> experimenters tell you that it works. Many Worlds can tell you why it works
> and why you need it. *
>
> So you say.  But all attempts to derive it, assuming MWI, have failed.  I
> look forward to your paper.
>
>
> *And unlike Schrodinger's Equation your dice equation directly determines
> a probability*
>
> Not as directly as Schrodinger's equation determines QM proability
> amplitudes.
>
> *; classical physics doesn't have or need a counterpart to the Born Rule
> (although the square of the absolute value of an electromagnetic wave is
> proportional to its energy). Classical physics can provide us with an
> excellent approximation of how the orientation of the die will change in
> time, so why do we need to use probability? The reason for that is
> practical not fundamental, sometimes in classical physics tiny changes in
> initial conditions lead to exponentially diverging trajectories over time,
> and you're never going to know the initial conditions exactly, and even if
> you did you don't have the computing capacity to use them.*
>
> *> And you have no answer to what probability means, until you resort to
> "uncertainty of self-location",*
>
>
> *Resort to? If I'm not allowed to give the correct answer then my answer
> is going to be wrong. Many Worlds says everything always obeys
> Schrodinger's equation including the observer, therefore there will always
> be self-location uncertainty, it can't be avoided. *
>
> And how does that result in uncertainty, when you are located in every
> branch.  It's just the problem of what does probability mean when
> everything happens.  You're just pushing the problem around.
>
> Brent,
>
> The problem isn’t that "everything happens"—it’s *how often* different
> things happen from the perspective of an observer. Probability in MWI
> doesn’t mean "some branches exist and others don’t" but rather that an
> observer finds themselves in certain branches *proportionally* to their
> measure.
>
> Saying "you’re just pushing the problem around" ignores that probability
> in any framework is about *expectations for future experience* based on
> structure. In a single-world view, you justify probabilities by appeal to
> hypothetical ensembles or repeated trials that never actually happen. In
> MWI, the structure of the wavefunction provides the ensemble *within*
> reality, and measure determines where most instances of an observer exist.
>
> Also, I’m not specifically advocating for MWI. I lean more towards *a
> computational theory of reality*, where measure and probability emerge
> from an underlying informational structure. But I do favor frameworks where 
> *everything
> happens* rather than a single unique history set in stone forever.
>
> *Then you'll like this: *
> *In a horse race, according to the MWI, multiple worlds come into
> existence for all possible winners in a particular race. But for one given
> race, are there are not multiple worlds, possibly countably infinite, which
> come into existence for every possible way in which the winner wins, while
> retaining the finishing order of the losing horses? I think so, and is the
> reason I find the MWI and its devotees, lacking in discrimination. But for
> a discerning eye, it's in the eye of the beholder, of Schrodinger's
> equation. AG  *
>
>
> AG,
>
> That’s exactly the point, MWI doesn’t just split for the winner, it splits
> for every possible microscopic detail of the race, including variations in
> how each horse crosses the finish line, fluctuations in the crowd, air
> molecules, and so on. The number of branches isn’t just countably infinite;
> it follows the continuous evolution of the wavefunction.
>
> But calling that "lacking in discrimination" misses the core idea. It’s
> not about choosing which worlds are "important", it’s about unitary
> evolution preserving all possible outcomes. The structure is dictated by
> Schrödinger’s equation, not by human intuition about what "should" count as
> a distinct event.
>
> If you think that level of detail makes MWI unreasonable, you should also
> reject classical probability, where every possible dice roll, coin flip, or
> weather pattern is part of a notional ensemble. The only difference is that
> MWI doesn’t assume unrealized outcomes "disappear" without explanation.
>
> Quentin
>
>
> *So every wiggle of your finger or toe results in perhaps uncountable
> worlds coming into existence, as well as every random turn of a flying
> insect? It just doesn't pass the smell test. AG *
>
>
> AG,
>
> Yes, every quantum interaction leads to branching—whether it’s a photon
> reflecting off your skin or an insect flapping its wings. But the mistake
> is thinking of this as “new worlds popping into existence.” MWI doesn’t add
> anything extra, it simply follows unitary evolution, where all possible
> outcomes exist in superposition.
>
> What doesn’t pass the smell test is the idea that only one history is
> mysteriously “chosen” while the rest, dictated by the same Schrödinger
> equation, vanish without explanation.
>
>
> What's the difference between an outcome not realized, and a branch which
> is disjoint from this world (and BTW, what is a branch)? AG
>

AG,

An unrealized outcome in a single-world interpretation means it never
happened, it was just a hypothetical, a calculation tool that never
manifested in reality. In MWI, an alternative outcome is not "unrealized"
but real in a disjoint branch, it exists, but in a different part of the
wavefunction that no longer interferes with ours.

A branch is simply a part of the universal wavefunction that has decohered
from others due to interactions with the environment. Once decoherence
happens, branches stop interfering, effectively behaving as separate
classical-like worlds.

So the key difference is: in single-world views, unrealized outcomes are
fiction, never happened,  never will, never experienced, never interacted;
in MWI, they are real but inaccessible due to decoherence.

Quentin


>
> If you accept quantum mechanics, you already accept that reality operates
> in a way that defies classical intuition. Rejecting MWI because it feels
> excessive is just favoring one form of weirdness over another.
>
> Quentin
>
>
>
> Saying 'some things happen and others don’t, just because' is not an
> explanation—it’s an arbitrary assertion, no better than saying 'God did it
> that way.' A real theory should provide a mechanism for why certain things
> are observed rather than simply declaring them to be the case.
> Quentin
>
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