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- Xref: sparky sci.physics:21720 alt.sci.physics.new-theories:2602
- Newsgroups: sci.physics,alt.sci.physics.new-theories
- Path: sparky!uunet!well!sarfatti
- From: sarfatti@well.sf.ca.us (Jack Sarfatti)
- Subject: Peer review of Budnik's "delays" in Aspect's test of Bell.
- Message-ID: <Bzr4LI.FL@well.sf.ca.us>
- Sender: news@well.sf.ca.us
- Organization: Whole Earth 'Lectronic Link
- Date: Thu, 24 Dec 1992 06:56:06 GMT
- Lines: 200
-
-
- Sarfatti responds to:
- *...* enclose my comments on Budnik
- From: paul@mtnmath.UUCP (Paul Budnik)
- Subject: Re: PS on Budnik's "delay" in Bell's inequality test.
- Date: 23 Dec 92 16:11:48 GMT
-
- In article <1992Dec22.145056.1452@lmpsbbs.comm.mot.com>,
- bhv@areaplg2.corp.mot.c
- om (Bronis Vidugiris) writes:
- > In article <BzHLnr.GK2@well.sf.ca.us> sarfatti@well.sf.ca.us (Jack
- Sarfatti) writes:
-
- > I looked again trying to understand what is exciting Budnik so much. Does
- he not know that Aspect's experiment in 1982 has polarization orientation
- switching times that were short compared to photon flight times from source
- to detectors. So that the nonlocal correlation of (cos@)^2/2 that violates
- Bell's locality inequality is definitely observed across spacelike
- intervals.
-
- This is not correct.
-
- *Paul, I'm sure Alain Aspect would not agree with you! Aspect stayed with
- me in San Francisco a few years ago. He said all his attempts to think of
- how to communicate on the connection failed because of unitarity - it is
- significant that he did try! No doubt our Dostoyevskian Grand Inquisitor
- Senor Baez and his fellow Friars would label him a "crackpot" for daring to
- think such heresy!*
-
- There was no *direct* measurement in Aspect's experiment of the delay
- between when a particle traversed the polarizer and was detected.
-
-
- *OK, Paul, now at least I am beginning to see what the hell you are talking
- about in "delays" - you were not very clear before and I am not the only
- one you confused. Let's try to picture your above remark in terms of a
- spacetime diagram. Your key phrase is:
-
- "the delay between when a particle traversed the polarizer and was
- detected"
-
- In my analysis this delay is negligible (i.e. short compared to flight
- times from source to polarizer) and essentially irrelevant. Why do you
- think it important?
-
- 4 5
- \ /
- \ /
- \ 2 3 /
- \ /
- \ /
- \ /
- \ /
- \ a b /
- \ /
- \ /
- \/
- 1
-
- 1 = pair source emission event
- 2(3) = scattering of photon a(b) from polarizer A(B)
- 4(5) = irreversible absorption of scattered photon a(b) by detectors A'(B')
-
- So Budnik's delays are 24 and 35 for photon pair a,b emitted from event 1.
- For simplicity make everything symmetrical on each side. Suppose only one
- photon pair through the system during a measurement. Now suppose each
- photon wave packet has time width T1. Let's also suppose that the time of
- flight of a surface of constant phase of the photon probability wave
- through the thickness of each polarizer is T2. Suppose the polarizer is
- rotating at angular rare w. Suppose T1<<T2, then the angular uncertainty
- d@(2(3)) is wT2. In the other extreme, if T1>>T2 the angular uncertainty is
- wT1. Good measurements require that the angular uncertainty be small
-
- d@(2(3)) << @(2,3)
-
- compared to angle @(2,3) defined as the nonlocal parameter
-
- @(2,3) = @(2) - @(3)
-
- the space-time interval 23 is spacelike in Aspect's experiment because of
- the fast acoustic switches (the switching times in @(2(3)) are short
- comapred to 12(3). In fact the ideal correlation of sqm of
- (cos(@(2,3))^2/2 is independent of 23 frame invariant metric distance. What
- possible relevance can 24 or 35 have to the basic idea of Aspect's
- experiment? So far, Budnik I fail to see where the problem is. Perhaps,
- someone else sees the problem? Does anyone else see what Budnik sees? Well
- let's continue.*
-
-
- Aspect estimated delays based on assumptions about flight time.
-
- *What does this mean? Anyone else understand what this means?*
-
- Such assumptions
-
- *What assumptions? State them!*
-
- are not in general valid in QM.
-
- You cannot know where a particle is at a given time unless you observe the
- particle at that time.
-
- *I agree with the above abstract remark but fail to see how it is relevant
- to the concrete question at issue. Does any one else recognize how it is
- relevant?*
-
- See J. D. Franson, Physical Review D, pgs. 2529-2532, Vol. 31, No. 10, May
- 1985 for a detailed analysis of this issue.
-
- *It would help if you could summarize what you understand Franson is doing
- and show clearly how it relates to your idea which so far eludes me.*
-
- If that is his concern then the answer is simple. But it seems to
- be something else- he says the "delay" can be measured but he does not give
- a clear and complete procedure so that I conclude it is much ado about
- nothing. I would like to be proved wrong in this opinion if any one else
- thinks they understand Budnik's idea.
-
- The way you measure the delay is by varying the polarizers between states
- that maximize and minimize the probability of joint detections.
-
- *The probability of joint detection is (cos@)^2/2 so that @ = 0 is max and
- @ = pi/2 is min. That much I understand. But I do not understand in
- operational terms "measure the delay is by varying the polarizers between
- states". Do you mean switching from 0 to pi/2 between arrivals of
- successive photon pairs. Aspect certainly does the equivalent of that given
- less than ideal conditions -but how does that relate to 24 and 35 in above
- diagram which is a literal translation of your explicit statement?*
-
- You then directly measure the time delays between when you have changed the
- polarizers and when this affects the probability of a joint detection.
-
- *This seems to be delusional word salad - totally meaningless in
- operational terms. Now I may be being stupid here, but does anyone else see
- what Budnik is driving at? What does it mean and how does it realte to his
- earlier remark "There was no *direct* measurement in Aspect's experiment of
- the delay between when a particle traversed the polarizer and was detected?
- "
-
-
- This is a technically more difficult experiment than Aspect's.
-
- * Difficult indeed because it is apparently meaningless.*
-
- Since you cannot control when a photon traverses the polarizer the delays
- will be dominated by the lack of synchronization between when a photon is
- emitted and when a polarizer changes state.
-
- *This remark makes some sense, but it has no logical connection to "There
- was no *direct* measurement in Aspect's experiment of the delay between
- when a particle traversed the polarizer and was detected."
-
- Although,"Since you cannot control when a photon traverses the polarizer
- the delays will be dominated by the lack of synchronization between when a
- photon is emitted and when a polarizer changes state." makes some sense it
- is wrong. First of all, a good experimenter will make sure that each
- polarizer is steady when each photon wave-packet is scattering from it.
- The wave packet widths are small compared to the distances 12 and 13 - and
- the whole point of the coincidence circuitry is to make Budnik's point
- wrong.*
-
- You can minimize this by emitting photons at a rapid rate, but the rate
- cannot be too high or you will not be able to distinguish joint detections
- from the detection of two photons from different photon pairs. These
- problems can be dealt with by increasing the total distance between the
- photon source and detectors. This introduces additional technical problems.
- I do not know how difficult such an experiment would be, but it is
- certainly doable in theory. That is all this is needed to prove my claim
- that quantum mechanics is an incomplete theory.
-
- I'm curious too - I checked and I don't have ready access to the reference
- > Paul cites and I haven't followed up 'special ordering' it from our
- library. One concern I had in thinking back over the experiment was the
- delay between the emission of the cascade photons. [I assume Aspect used
- cascade photons.]
-
- Aspect measured the times between joint detections and depended on the
- geometry of the experiment and the flight time of photons to estimate the
- delays. Franson argued that this was not legitimate.
-
- *Really, then give relevant quotes by Franson.
-
- The delays could have been as long as the excited states of the atom
- emitting the photon or even as long as the coherence times of the lasers
- used to excite the atoms.
-
- *Surely, both these obvious delays were well understood by Aspect and taken
- into account by him. The main reason its so hard to understand what you are
- babbling about is that you keep pulling the rug out from under us in the
- meaning of "delays" How do the "delays" of the above paragraph square with
- the meaning of "delays" in ""the delay between when a particle traversed
- the polarizer and was detected"? Budnik is, by implication attacking
- Aspect's competence. It would be good for Aspect to respond to Budnik.
- Like Pontius Pilate I wash my hands of this and ask "What is truth?" I have
- not changed my opinion that Budnik has no real physics here - my verdict is
- "BOGUS!" - to the cross!*
-
-
-
-
-