On 5/19/2025 8:39 PM, Alan Grayson wrote:


On Monday, May 19, 2025 at 6:57:57 PM UTC-6 Brent Meeker wrote:



    On 5/19/2025 3:00 PM, Alan Grayson wrote:


    On Monday, May 19, 2025 at 12:22:29 AM UTC-6 Brent Meeker wrote:



        On 5/18/2025 9:58 PM, Alan Grayson wrote:


        On Sunday, May 18, 2025 at 4:16:26 PM UTC-6 Brent Meeker wrote:



            On 5/18/2025 10:02 AM, Alan Grayson wrote:


            On Tuesday, May 13, 2025 at 4:54:55 AM UTC-6 Alan
            Grayson wrote:

                On Monday, May 12, 2025 at 4:15:52 PM UTC-6 Brent
                Meeker wrote:



                    On 5/12/2025 1:58 PM, Alan Grayson wrote:


                    On Friday, May 9, 2025 at 10:40:42 PM UTC-6
                    Brent Meeker wrote:

                        On 5/9/2025 7:08 PM, Alan Grayson wrote:
                        *I can see that the measurement spreads
                        due to instrument limitations are usually
                        immensely larger than the much smaller
                        spreads accounted for by the UP, but what
                        causes these much smaller spreads? Is
this a quantum effect? AG*

                        Yes.  Quantum evolution is unitary, i.e.
                        the state vector just rotates in a complex
                        Hilbert space so that probability is
                        preserved.  Consequently the infinitesimal
                        time translation operator is U=1+e6/6t or
                        in common notation 1-i(e/h)H where
                        H=ih6/6t and h is just conversion factor
                        because we measure energy in different
                        units than inverse time. It's not
                        mathematics, but an empirical fact that h
                        is a universal constant.

                        Brent


                    *If one wants to prepare a system in some
                    momentum state to be measured, doesn't this
                    imply a pre-measurement measurement, *
                    Right, given that it's an ideal measurement. 
                    Most measurements don't leave the system in the
                    eigenstate that is the measurement result.  An
                    ideal measurement is one that leaves the system
                    in the state that the measurement yielded.


                    *and the observable to be measured remains in
                    that state on subsequent measurements? *
                    Only if they're ideal measurements of that same
                    variable or of other variables that commute
                    with it.


                    *If so, how can the unitary operator, which
                    just changes the state of the system's wf,
                    create the quantum spread? *
                    You don't need a change in the wf to "create
                    the quantum spread".  Having prepared in an
                    eigenstate of A just measure some other
                    variable B that doesn't commute with A.  In
                    general A will be a superposition of other
                    variables, say A=xC+yD; that's just a change of
                    coordinates. But the system is not in an
                    eigenstate of C or D.

                    Brent


                *Sorry, I really don't get it. Not at all! If we
                want to prepare a particle with some momentum p,
                why would we measure it with some non-commuting
                operator, and why would this, if done repeatedly,
                result in a spread of momentum? And what has this
                to do with a unitary operator which advances time?
                TY, AG *

            *
            *
            *Is the spread in momentum caused by an imprecision in
            preparing a particle in some particular momentum?
            Generally speaking, how is that done? TY, AG
            *
            *The HUP doesn't limit how precisely you can prepare a
            particle's momentum. The HUP just says that the more
            precisely the momentum is determined the less precisely
            defined will be the conjugate position. *


        *I know. What I don't know is the cause of the spread. AG*

        *See attached.

        Brent*



    *Your attachment shows how to establish the HUP, not why there is
    a spread in momentum. Classically, energy and momentum are
    related by a simple formula. So if one wants to /prepare/ a
    system in some specific momentum, one needs to control the energy
    of the particle. Presumably, this can never be done precisely;
    hence we get the spread. Is this not a sufficient explanation for
    the spread? AG*

    *As far as the HUP is concerned the cause of spread in momentum is
    that the spread in conjugate position must be finite, and vice
    versa. *


*Are all the momenta in the spread, eigenvalues of the momentum operato*r*? AG*
*Yes.  But they have different probabilities of being found when measured.

Brent*

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