Re: Quantum Rebel

2004-08-12 Thread Jesse Mazer
Russell Standish wrote:
On Thu, Aug 12, 2004 at 01:08:36AM -0400, Jesse Mazer wrote:
Also notice that in the analysis of Afshar's experiment by W. Unruh at
http://axion.physics.ubc.ca/rebel.html which scerir linked to, Unruh does
not dispute Afshar's claim that all the photons from the each pinhole end
up in a single detector. In fact, he offers a simpler version of the
experimentquot; involving a multiple pass interferometer, depicted in 
figure 2,
and says that in this experiment you do know which path a photon took by
looking at which detector it hits: By measuring which detector they
triggered, 5 or 6, one measures which of the beams, 1 or 2, the photon
traveled along. Since the experiment in figure 2 is just supposed to be a
simpler version of Afshar's experiment, it's pretty clear that Unruh
would not disagree that the lens insures that knowing which detector
absorbed a photon is enough to tell you which path the photon must have
taken through the pinholes. Unruh is a fairly big-name physicist and his
explanation of what's wrong with Afshar's conclusions about 
complementarity
are pretty detailed, while I don't know anything about Basil Hiley and his
criticisms are more vague.
After looking at Unruh's explanation, I can only say that he puts in a
very persuasive manner, the substance of my post to this list: namely
that the insertion of a diffraction grating (equiv. Unruh's path 4
absorber) destroys the which-way information.
Hmm, on rereading the last section of Unruh's article I see you're 
correct--in the second-to-last paragraph he says However, while in the 
interference experiment, the presence or absence of the absorber in path 4 
would seem to make no difference-- no photons travel along path 4 to be 
absorbed-- it makes a crucial difference in the interpretation. A critical 
part of the the interpretation is drawing the inference that IF the particle 
was detected in detector 5, THEN it must have come from path 1. Similarly, 
IF it was detected in detector 6, then it came from path 2. The presence of 
the absorber in path 4 does not change the experiment, but it destroys these 
inferential chains.

I'm a little confused by his answer though, because he says the presence or 
absence of the absorber along path 4 in figure 2 makes absolutely no 
difference to the outcome of the experiment, since interference insures no 
photons would travel along path 4 even without the absorber there. So if you 
placed a continuous screen in the position of the two detectors, you'd still 
get two distinct spots with no interference fringes between them...and 
doesn't complementarity say that the absence of interference between two 
spots on a screen in the double-slit experiment can only occur when you *do* 
know which hole the photons landing on each spot went through?

Along the same lines, I'm confused about exactly how your answer fits with 
Unruh's answer. You said:

Now in the article, Afshar claims to have measured which slit the
photon passed through and verified the existence of an interference
pattern. However, this is not the case - without the wires in
place to detect the presence of the interference pattern, photons
arriving at detector A have passed through slit A, and vice-versa with
detector B and slit B. However, with the wires in place, some photons
are scattered, indeed some photons which passed through slit A will
arrive at detector B. With both slits open, and the wire placed
exactly at a null point of the interference pattern, the photons
passing through slit A and arriving at detector B exactly counteracts
the photons passing thoguh slit B that have been lost through
scattering. The mathematics of quantum mechanics assures this,
coincidental this may seem.
Is Unruh saying that in figure 2 without the absorber, the amplitude of a 
photon travelling along path 4 is zero, but with the absorber in place, 
there is some nonzero amplitude for a photon to travel along path 4 but then 
be scattered into the wrong detector? If he's not suggesting the 
possibility the absorber will scatter photons without absorbing them is 
relevant here, then I wouldn't think he'd say the possibility the wires will 
scatter photons without absorbing them is relevant to Afshar's experiment. 
When you say the mathematics of quantum mechanics assures this, did you 
actually do a calculation of the effects of scattering in Afshar's 
experiment?

Jesse Mazer



Re: Quantum Rebel

2004-08-12 Thread scerir
From: John Collins
 
 Essentially Ashfar's experiment involves fooling himself 
 (and perhaps a few others) with a new single-path photon 
 thoery, then undermning the new theory, whcih was not quantum
 mechanics..

The orthodox QM says that if we have the usual two-slit,
a which way detector, and the screen, the interference
pattern is destroyed as soon as the detector finds (with
probability 1) the which way. In principle this is true 
also in the case of single particles. In practice you need 
many particles. (If the detector finds the which way with
probability  1, the interference pattern is destroyed
partially, because there is a Greenberger  Yasin equation,
and so on ...).

The orthodox QM also says that is we put a which way eraser
between the (working) which way detector and the screen, 
the interference pattern is restored. But where it is restored?
At the screen of course.

Now in the Afshar experiment those lenses are (supposed to be)
which way detectors. Now if we insert, after each of those lenses,
the which way eraser, an interference pattern - according to
orthodox QM - will be restored. But where it will be restored?
At the screen (here - in Afshar exp. - I do not know if there is 
a screen, but in principle it could be so).

It seems to me that the which way eraser affects what happens
after, but does not affect what already happened before. But
if that is true for the which way eraser, it must be true
also for the which way detector. That is to say that any which
way detector does affect what happens after but does not
affect what already happened before.

If the above is true - but I doubt it, since here is late, hot, and
dark ! - assuming (as Afshar/Cramer) that those lenses (which way 
detectors) should affect what already happened before, at
those little wires level, is not solid at all. 

s. 

Btw, it is not so simple to define complementarity.
Between waves (are there waves in Matrix Mechanics?) and 
particles? Between localization and superposition of amplitudes 
(von Weizsaecker)? Between interference pattern and which way 
knowledge? Between continuous and discontinuous? Between 
separability and unitarity? Between reversibility and 
irreversibility? This one seems to be close to what Lawrence Bragg 
said: Everything in the future is a wave, everything in the past 
is a particle!