From: mpc755 on
On May 9, 2:39 pm, Esa Riihonen <e...(a)riihonen.net.not.invalid> wrote:
> mpc755 kirjoitti:
>
> > Post a link to the experiment or keep your baseless assumptions to
> > yourself.
>
> This is quite basic and easy experiment, so it would be quite strange if
> no one would have done it. Turns out the issue was studied already almost
> two hundred years ago - see Arago-Fresnel laws.
>
> [0]
> But anyways, here is one recent experiment:http://arxiv.org/abs/1003.2729
>
> Specifically see the figure 3 on page 5.
>
> Now that the prediction of your aether theory (actually your declaration,
> supposedly somehow based on the theory), namely that L and R light will
> produce differing interference patterns, has been experimentally shown
> wrong we will do as any sane scientist will do: scrap the theory and start
> something new - right?
>

'Generalized Arago-Fresnel laws: The EME-flow-line description'
http://arxiv.org/abs/1003.2729

"The results of Fig. 2 seem to indicate a slight polarization
dependent transversal shift. This could be traced back to a systematic
beam displacement during adjustments of the Babinet compensator. The
results of Fig. 3 were obtained after resolving this problem. Fig. 2 —
and more convincingly Fig. 3— show that the interference pattern does
not depend on the state of polarization of the incident laser light."

Polarization dependent transversal shift is exactly what I predicted.

The interference pattern depends on the state of the polarization of
the incident laser light. The experimenters incorrectly adjusted the
Babinet compensator to get their desired results.

From the original article the article you linked to was derived from:

'Double-slit quantum eraser'
http://grad.physics.sunysb.edu/~amarch/Walborn.pdf

"Suppose that in front of each slit we place a quarter-wave plate,
with the fast axis at an angle of 45° (or -45°) with respect to the
photon polarization direction. Upon traversing either one of the wave
plates, the photon becomes circularly polarized, and acquires a well-
defined angular momentum. Supposing that the wave plate is free to
rotate, it should acquire an angular momentum opposite to that of the
photon, and rotate right or left, depending on the chirality of the
photon."

The quarter-wave plates in front of each slit cause there to be two
interference patterns created at detector Ds. One associated with the
right photons and one associated with the left photons. The cumulative
coincidence counts of the two interference patterns results in Fig 7.

"Experimentally, this can be done by placing a polarizer in the path
of beam p and orientating it at +45° to select [|+>p] or at -45° to
select [|->p]. The interference pattern is recovered through the
coincidence detection of photons s and p. Notice that the fringes
obtained in the two cases are out of phase. They are commonly called
fringes and antifringes."

The placement of the polarizer in the path of beam p discerns the two
interference patterns created at detector Ds.

Cumulative coincidence counts of Fig. 4 and Fig. 5 result in Fig. 7.
From: Esa Riihonen on
mpc755 kirjoitti:

> On May 9, 2:39 pm, Esa Riihonen <e...(a)riihonen.net.not.invalid> wrote:
>> mpc755 kirjoitti:
>>
>>
>> > Post a link to the experiment or keep your baseless assumptions to
>> > yourself.
>>
>> This is quite basic and easy experiment, so it would be quite strange
>> if no one would have done it. Turns out the issue was studied already
>> almost two hundred years ago - see Arago-Fresnel laws.
>>
>> [0]
>> But anyways, here is one recent
>> experiment:http://arxiv.org/abs/1003.2729
>>
>> Specifically see the figure 3 on page 5.
>>
>> Now that the prediction of your aether theory (actually your
>> declaration, supposedly somehow based on the theory), namely that L and
>> R light will produce differing interference patterns, has been
>> experimentally shown wrong we will do as any sane scientist will do:
>> scrap the theory and start something new - right?
>>
>>

Once again you constructed several (seven) answers in little over 5 hours
to the same post of mine - what is the problem ADHD. I guess based on the
time label this is your best reply.


> 'Generalized Arago-Fresnel laws: The EME-flow-line description'
> http://arxiv.org/abs/1003.2729

This is a reference to the abstract of the paper - why not use the link
to the full paper given above.

> "The results of Fig. 2 seem to indicate a slight polarization dependent
> transversal shift. This could be traced back to a systematic beam
> displacement during adjustments of the Babinet compensator. The results
> of Fig. 3 were obtained after resolving this problem. Fig. 2 — and more
> convincingly Fig. 3— show that the interference pattern does not depend
> on the state of polarization of the incident laser light."
>
> Polarization dependent transversal shift is exactly what I predicted.

I'm afraid you didn't predict any 'tranversal' shift. Actually anyone
that has actually done diffraction experiments (as I have BTW) knows
quite well that the transversal (or any other direction) placement of the
pattern depends on the alignment of the equipment. All you have here is a
minor effect due to the misalignment on top of the strong signal in first
of the experiments, so minor that it can't even be seen from the picture.
A small effect that is completely absent from the later experiments after
the realignment. BTW I'm not sure that you noticed but these guys are
actually in 'your camp' - they use the 'Bohmian' EME-flow line
description of the setup.

> The interference pattern depends on the state of the polarization of the
> incident laser light. The experimenters incorrectly adjusted the Babinet
> compensator to get their desired results.

Hah. Once again, this adjustment was capable of destroying the whole
effect for all the polarization states - I guess you "predicted" that
also ;)

> Figures 3 and 4 better are a better representation of the effect:
>
> 'A Delayed Choice Quantum Eraser'
> http://arxiv.org/PS_cache/quant-ph/pdf/9903/9903047v1.pdf

I think we have seen this reference already. The paper and the associated
figures are related to the quantum erasure experiment and have nothing to
do with the experimentally separate discussion whether the polarization
state affects the diffraction pattern - it doesn't. I think you are quite
confused and desperate.

It is quite obvious at this point that your aether "theory" is nothing
but hot air verbiage, and it is totally meaningless to continue this
"discussion".

I have a suggestion though. As you are operating under a nym you have
always the option for disappearing from here for a while. You could use
the saved time for actually studying physics - for a couple of years at
least. After that you could come back with a new nym and avoid the most
embarrassing statements like "atomic clock tick rate is affected by the
aether pressure on the nucleus" and other stupidities.

And for a bonus, here is a more or less clear headed and respectable
challenge on the interpretation quantum erasure (at least it looks
respectable to me - others more knowledgeable might know better). Before
you can produce anything even remotely at that level, you have no change
of having anyone to take you seriously here.

http://dx.doi.org/10.1080/09500340701639953


Over and out,

Esa(R)

--
If starving people will be taught to pray instead of search for food,
famine would be over in a few weeks. -- Kaj Stenberg
From: mpc755 on
On May 18, 2:14 pm, Esa Riihonen <e...(a)riihonen.net.not.invalid>
wrote:
> mpc755 kirjoitti:
>
> > 'A Delayed Choice Quantum Eraser'
> >http://arxiv.org/PS_cache/quant-ph/pdf/9903/9903047v1.pdf
>
> I think we have seen this reference already. The paper and the associated
> figures are related to the quantum erasure experiment and have nothing to
> do with the experimentally separate discussion whether the polarization
> state affects the diffraction pattern - it doesn't. I think you are quite
> confused and desperate.
>

The polarization state affects the diffraction pattern. That is what
the article refers to as fringes and anti-fringes.

'Double-slit quantum eraser'
http://grad.physics.sunysb.edu/~amarch/Walborn.pdf

"Suppose that in front of each slit we place a quarter-wave plate,
with the fast axis at an angle of 45° (or -45°) with respect to the
photon polarization direction. Upon traversing either one of the wave
plates, the photon becomes circularly polarized, and acquires a well-
defined angular momentum. Supposing that the wave plate is free to
rotate, it should acquire an angular momentum opposite to that of the
photon, and rotate right or left, depending on the chirality of the
photon."

The quarter-wave plates in front of each slit cause there to be two
interference patterns created at detector Ds. One associated with the
right photons and one associated with the left photons. The cumulative
coincidence counts of the two interference patterns results in Fig 7.

"Experimentally, this can be done by placing a polarizer in the path
of beam p and orientating it at +45° to select [|+>p] or at -45° to
select [|->p]. The interference pattern is recovered through the
coincidence detection of photons s and p. Notice that the fringes
obtained in the two cases are out of phase. They are commonly called
fringes and antifringes."

The placement of the polarizer in the path of beam p discerns the two
interference patterns created at detector Ds.

Cumulative coincidence counts of Fig. 4 and Fig. 5 result in Fig. 7.