On 5/19/2025 9:03 PM, Alan Grayson wrote:


On Monday, May 19, 2025 at 9:55:36 PM UTC-6 Brent Meeker wrote:



    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*


*But if one always gets a spread, how can any particular momentum in the spread be measured? AG
*
*You can't choose which value you get measuring a random variable.  You just measure momentum and you get a certain value. Then you repeat the experiment and you get a different value.  You repeat this a thousand times and you can plot the distribution function of momenta and measure the spread.

Brent*

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