On Fri, Oct 18, 2019 at 6:20 PM 'Brent Meeker' via Everything List <
[email protected]> wrote:

> 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]> 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]> 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.
>

OK. If you recombine the beams before decoherence, you effectively erase
the first erasing measurement. In which case the interference pattern
disappears, and the second up-down measurement doesn't do anything except
but show the diffraction patterns from each slit separately. (up-down
distinguishes the L-R slits -- you know which-way!)

Bruce

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