On 7/30/2018 9:21 PM, [email protected] wrote:


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



    On 7/30/2018 4:40 PM, [email protected] <javascript:> 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.

*And for this reason I still conclude that Schroedinger correctly pointed out the fallacy in the standard interpretation of superposition; namely, that the system represented by a superposition, is in all components states simultaneously. AG
*

It's not a fallacy.  It just doesn't apply to the cat or other macroscopic objects, with rare laboratory exceptions.  Any old plane polarized photon can be represented as being in a superposition of left and right circular polarization.  It is */not/* the case that a system is in all basis states at once unless you count being in state /|x>/  with zero amplitude as being in /x/.

Brent


    **
    Brent

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