On 8/1/2018 4:49 AM, Bruno Marchal wrote:

On 1 Aug 2018, at 07:49, Brent Meeker <meeke...@verizon.net <mailto:meeke...@verizon.net>> wrote:



On 7/31/2018 10:19 PM, Jason Resch wrote:


On Tue, Jul 31, 2018 at 4:52 PM Brent Meeker <meeke...@verizon.net <mailto:meeke...@verizon.net>> wrote:



    On 7/31/2018 2:38 PM, Jason Resch wrote:


    On Tuesday, July 31, 2018, Brent Meeker <meeke...@verizon.net
    <mailto:meeke...@verizon.net>> wrote:



        On 7/31/2018 9:46 AM, Jason Resch wrote:


        On Tue, Jul 31, 2018 at 1:11 AM Brent Meeker
        <meeke...@verizon.net <mailto:meeke...@verizon.net>> wrote:



            On 7/30/2018 9:21 PM, agrayson2...@gmail.com
            <mailto:agrayson2...@gmail.com> wrote:


            On Tuesday, July 31, 2018 at 1:34:58 AM UTC, Brent
            wrote:



                On 7/30/2018 4:40 PM, agrays...@gmail.com wrote:


                On Monday, July 30, 2018 at 7:50:47 PM UTC,
                Brent wrote:



                    On 7/30/2018 8:02 AM, Bruno Marchal wrote:
                    *and claims the system being measured is
                    physically in all eigenstates
                    simultaneously before measurement.*


                    Nobody claims that this is true. But most
                    of us would I think agree that this is what
                    happens if you describe the couple
                    “observer particle” by QM, i.e by the
                    quantum wave. It is a consequence of
                    elementary quantum mechanics (unless of
                    course you add the unintelligible collapse
                    of the wave, which for me just means that
                    QM is false).

                    This talk of "being in eigenstates" is
                    confused.  An eigenstate is relative to some
                    operator.  The system can be in an
                    eigenstate of an operator. Ideal
                    measurements are projection operators that
                    leave the system in an eigenstate of that
                    operator.  But ideal measurements are rare
                    in QM.  All the measurements you're
                    discussing in Young's slit examples are
                    destructive measurements. You can consider,
                    as a mathematical convenience, using a
                    complete set of commuting operators to
                    define a set of eigenstates that will
                    provide a basis...but remember that it's
                    just mathematics, a certain choice of
                    basis.  The system is always in just one
                    state and the mathematics says there is some
                    operator for which that is the eigenstate.
                    But in general we don't know what that
                    operator is and we have no way of physically
                    implementing it.

                    Brent


                *I can only speak for myself, but when I write
                that a system in a superposition of states is in
                all component states simultaneously, I am
                assuming the existence of an operator with
                eigenstates that form a complete set and basis,
                that the wf is written as a sum using this
                basis, and that this representation corresponds
                to the state of the system before measurement. *

                In general you need a set of operators to have
                the eigenstates form a complete basis...but OK.

                *I am also assuming that the interpretation of a
                quantum superposition is that before
                measurement, the system is in all eigenstates
                simultaneously, one of which represents the
                system after measurement. I do allow for
                situations where we write a superposition as a
                sum of eigenstates even if we don't know what
                the operator is, such as the Up + Dn state of a
                spin particle. In the case of the cat, using the
                hypothesis of superposition I argue against, we
                have two eigenstates, which if "occupied" by the
                system simultaneously, implies the cat is alive
                and dead simultaneously. AG *

                Yes, you can write down the math for that.  But
                to realize that physically would require that the
                cat be perfectly isolated and not even radiate IR
                photons (c.f. C60 Bucky ball experiment).  So it
                is in fact impossible to realize (which is why
                Schroedinger considered if absurd).

            *
            CMIIAW, but as I have argued, in decoherence theory
            it is assumed the cat is initially isolated and
            decoheres in a fraction of a nano second. So, IMO,
            the problem with the interpretation of superposition
            remains. *

            Why is that problematic?  You must realize that the
            cat dying takes at least several seconds, very long
            compared to decoherence times.  So the cat is always
            in a /*classical*/ state between |alive> and |dead>.
            These are never in superposition.

            *It doesn't go away because the decoherence time is
            exceedingly short. *

            Yes is does go away.  Even light can't travel the
            length of a cat in a nano-second.



        What if the cat is on Pluto for this one hour?  Would it
        not be perfectly isolated from us on Earth, and thus
        remain in a superposition until the the several hours it
        takes for light to get to Earth from Pluto reaches us?

        ?? Are you assuming that decoherence only occurs when
        humans (or Earthlings) observe the event?


        Brent



     No, just that superposition is a relative, rather than
    objective notion.

    OK.  Welcome to QBism.


After reading the wiki article on QBism I still can't say I understand what it is about, as it doesn't seem to offer any core positions.

I am an adherent of bayesianism, and believe it applies generally in all domains (being an agent having to make decisions/bets), so what does QBism add if one already accepts a general reliance on Bayes theorem?  It doesn't seem like QBism takes any strong position on any of the quantum paradoxes, nor offer any insights to addressing or explaining them.  In this it seems like a pretty empty theory, with hints towards the "instrumentalist" and "shut up and calculate" mindsets--that only the probability matters.  To the extent that is true, I reject QBism.  While QBism might not put forward anything that is false, the attitude it conveys seems like it would stymie progress towards advancing our understanding of reality.

QBism says that QM is a theory for predicting personal beliefs.  The "collapse" of the wave function is simply updating one's beliefs based on an observation.


That leads to the many-worlds, or its "many-minds” variants (even closer to what mechanism enforce on the interpretation of the observable). ITSTM.

There are many-minds who just happen to have (in many cases) different information about the world and so use different states or Hamiltonians to predict what they will observe.  But the evidence is that there is only one world.

Brent

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