On 10/17/2019 8:38 PM, Bruce Kellett wrote:
On Fri, Oct 18, 2019 at 2:08 PM 'Brent Meeker' via Everything List <[email protected] <mailto:[email protected]>> wrote:

    On 10/17/2019 4:34 PM, Bruce Kellett wrote:
    On Fri, Oct 18, 2019 at 10:05 AM 'Brent Meeker' via Everything
    List <[email protected]
    <mailto:[email protected]>> wrote:


        But I wonder what happens in Carroll's experiment if, after
        measuring in the left/right basis and noting that two
        different interference patterns can then be discerned by
        considering either those due to left spin recording particles
        or considering right spin particles, one measures the
        recording particles again in the up/down basis.  The overall
        pattern is the same, it's just that  you've relabeled spots
        on the screen according to whether the second measurement of
        recording particles assigned them to UP or to DOWN.  Now you
        can consider the subset labeled UP (or DOWN).  This should be
        a superposition of ensembles randomly selected from the left
        and right ensembles and in that case would not show an
        interference pattern...but the information has certainly been
        erased (twice)?


    If I understand you, what you are suggesting is that either the
    left polarized, or right polarized, are measured again in the
    up-down direction. I think that if you do this second
    measurement, you will simply reduce the intensity by a factor of
    two.

    No.  You just partitioning the spots on the screen in a different
    way, so there are the same number of spots. After the first
    measurement of the recording particles spins, in the left/right
    basis, you labeled the spots on screen according to left or
    right.  And when you looked only at the left labeled spots they
    showed an interference pattern.  And necessarily the right labeled
    spots were the complement relative to the no-interference pattern.
    So there are two implicit complementary interference patterns
    hidden in the no-interference pattern.  But on the second
    measurement of the recording particles in the up/down basis each
    one should be up or down with probability 1/2. So all those
    measuring UP is just a random selection of the overall ensemble,
    the ensemble that showed no interference.  So yes it's intensity
    is reduce (only half the spots end up labeled UP) but it's a
    no-interference pattern.

    The welcher weg information was permanently erased by the first
    left-right measurement.

    Right.  So why doesn't the interference pattern persist after the
    second measurement of the recording particles? I suppose the
    answer is that it does, we just don't have the information
    necessary to pick it out anymore.  Still it seems curious that we
    can erase the which-way once and, by looking at the results, find
    the interference pattern. But if we erase twice we can't find it.


Are you suggesting that we lose the original left-right labels? I thought that if you select 'left', then re-measure just those photons in the up-down basis, you still get the 'left' interference pattern, with the spots now randomly labelled 'up' or 'down'. If you put both the 'left' and 'right' photons through the second measurement, and lose the original labels, then the interference pattern may vanish, and you get randomly scattered 'up' and 'down' spots. But that is because you forgot the original separation -- it is still there, you just labelled things differently.

Or am I still missing your point?

I was thinking of the second, in which you do the two measurements in succession, like one SG after another so that you never looked at or recorded the first measurement result.  But that would mean you'd have to put the beams back together between the measurements.  In that case the second measurement would be just like the first hadn't happened, and you'd be able to discern an interference pattern.

Brent

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