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.  Of course as I pointed out there are usually much bigger causes just in classical sources of instrument uncertainties.

Brent*

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