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Yes, I generally had trouble understanding what you meant with that kind of statement.
DrChinese said:Just to add to my prior post: I think the situation could probably be formulated into an inequality using logic from Bell's Theorem.
Phrak said:Bell's inequality refutes quantum mechanics
jtbell said:How so?
DrChinese said:There is NO chance that a particular photon polarized at 0 degrees could pass through both a +45 polarizer and a -45 degree polarizer in the quantum mechanical view. The operative formula is the COS^2(L-R) rule, where L-R=90 degrees so that the result is 0 and there is no interference.
On the other hand, in the classical perspective, there IS a chance that any particular photon polarized at 0 degrees could pass through both a +45 polarizer and a -45 degree polarizer. Do you see why? The rule is different because the probability is resolved independently for each slit, unlike in the quantum view in which it is the relative angle of the L and R slits is important. So now you get COS^(L-0)*COS^(R-0) and there should be some interference because the result is .25 which is >0.
DrChinese said:Well at least you are thinking about it...
I would be interested in a demonstration of a classical wave effect which eliminates all interference when partial polarizers (or classical equivalent) are present in a setup similar to the double slit. You use the example of audio, and I think a careful consideration of your analogy will demonstrate that the interference will NOT be eliminated after all - as it would need to be to match light in a double slit.
Of course there is a lot more to the story on the quantum side anyway. If light were waves (only) then a lot of things would be different (in contradiction to experiment - see for example: http://people.whitman.edu/~beckmk/QM/grangier/Thorn_ajp.pdf" ). If light polarization operated as you imagine, things would be different with entangled particle pairs (in contradiction to experiment).
You may not be aware of all of the experiments out there (who is?), but you might want to at least ask before talking about the emperor's clothes. The double slit is just one piece of the puzzle.
Phrak said:You do realize that Bell's inequality refutes quantum mechanics, right?
DrChinese said:I am sure we agree that a violation of a Bell inequality refutes classical realism, and is consistent with QM. I simply think of the inequality as a boundary condition on (local) realism.
Frame Dragger said:I have to say that's a good way of putting it. I've been doing a good deal of reading on deBB, and a refresher on The TI, and more and more it seems that dBB and a few other theories are simply the ones that have not been swept aside by modern experimental evidence. dBB basically hinges on the QM being in violation of Bell's Inequalities, and not classical realism. The argument of (mechanical) bias in experiments such as a "2 channel" test, keeps dBB alive unlike most other theories which required LHV's.
However, the switch from locality to non-locality in dBB seems logically contrived for the sole purpose of maintaining a particular interpretation of reality as something other than emergent phenomena from a quantum soup of superpositioned probabilities. That doesn't make it wrong, and from everything I'm reading dBB can't be refuted right now and if nothing else it does a very good job of highlighting the huge gap in explaining how the microscopic and macroscopic worlds combine to form what we experience as reality in SQM. I think that the TI is probably on the right track, but it's hard to say that those theories, or MWI are more contrived than dBB.
...
The bottom line is that Bell kind of draws the line between the Classicist and SQM view of reality. It's a boundary in the common usage and not just the scientific term of art.
DrChinese said:I agree with what you are saying. dBB gets by because the context is non-local. Another interesting set of interpretations is the Time Symmetric group (including Relational BlockWorld RBW), in which a future context is allowed to influence the present. These have the "benefit" of being local, contextual (non-realistic) and time symmetric. Of course you swap one assumption for another, so whether the result is net better is a matter of preference.
mintparasol said:In the book he makes an example of the double slit experiment we all did in high school and says that if we fire one photon at the slitted screen, we'll get an interference pattern on the rear screen.
eaglelake said:If you fire one photon through the slits you will get one dot on the second screen. A single photon is always detected as a single particle (a dot), never as a wave. In fact, the single dot doesn’t reveal any wave properties. It is only when you detect many photons does the distribution of scattered photons begin to look like an interference pattern. There are sites on the web that show how the interference pattern is built up one photon at a time.
I am bothered that an author would make such a statement, but apparently it is all too common. No experiment has ever shown a particle behaving like a wave. The point is this – a quantum particle is not a wave.
Frame Dragger said:Annnnd... you're wrong. In fact, even when passing C60 or Rubidium atoms (one at a time) there is interference consistant with passage through both apertres of the experiment. There are sites on the web that show how 8th dimension lizards run the country... that doesn't make them accurate. Interference patterns of the type you describe are not consistant with a purely particle-theory of light. Light's wave-like properties are as well established as its particle-like properties.
As for experiment with photons... you'rre wrong again? I don't know what else to say... you can in fact set up simple controls for these experiements which eliminate interence by more than specifically polarized photons passng throuhg the apertures.
EDIT: Addition: "A quantum particle is not a wave." True. Photons are quanta which have wave and particle -like properties. They are neither waves, NOR particles and feel free to call them "quanta" not "quantum particles". That latter is... meaningless and semi-redundant.
eaglelake said:No need to be a wiseguy! If you do not understand something, just ask for a clarification.
I responded to the statement, “if we fire one photon at the slitted screen, we'll get an interference pattern on the rear screen.”, which is not true. A single photon is always detected as a single dot on the detection screen. A single photon is never smeared over the screen in an interference pattern, as a wave would be. If you want to see wave effects then you must repeat the same experiment many times.
The original statement by mintparasol referred to a single photon, while you are talking about, “passing C60 or Rubidium atoms (one at a time)”, which is about MANY atoms. “One at a time” means more than one! You seem to imply that the interference pattern is built up “one (atom) at a time”. I agree! That is exactly what I said. So, where is the disagreement?
The basic question is, “ When does a photon, or any quantum particle, look like a particle and when does it look like a wave”? We either observe one or the other, but never both at the same time. (Bohr’s complimentarity principle)
The answer is – if you detect a single particle it looks like a particle. It looks like a wave only after you have detected many of them. [1] (and, then, only in special circumstances.)
Best wishes.
[1] A. Tonomura, et al, Amer. J. Phys., 57, 117-120 (1989)
The fact that it takes multiple passes (as you say, a buildup) to make the pattern visible is a limitation of our detection methods.
Mentz114 said:FrameDragger:
I don't see how. A particle detector is designed to detect particles and that's what it does. What apparatus would you use to detect a 'Rubidium wave' ?
Frame Dragger said:The same way you do with buckyballs (C60) a la http://www.users.csbsju.edu/~frioux/two-slit/c60-slit.htm
Mentz114 said:That doesn't answer the question. The note you linked to shows the wave function that models the experiment. The wave function gives us probabilities of detecting the particle at certain locations. If you send one particle through, you detect one at the screen. If you send a 100 particles through one by one, they will make a pattern like the square of the wave function at the screen. The particle goes through one slit or the other but we cannot find out (even in principle) which slit, and still get the interference pattern building up.
I enjoyed that little note.
For more on single-photon interference look up Hong-Ou-Mandel.
mintparasol said:Thanks to all who've replied here. I think it's kind of cool that a question from someone like myself who has very little understanding of the technical aspects of QM can get such a lively debate going!
I've been reading and re-reading the thread and some of the links posted here and I think I have a slightly better understanding of what's going on here than I had at the beginning.
Thanks again
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But SQM is saying that the pattern is determined by the wave-function otherwise there would be no interference pattern. SQM does not say that the particles behave like classical particles.The belief the the pattern is simply a function of many particles acting without wave-like behaviour flies in the face of experimental evidence, but is compatible with non SQM or dBB theories. Even dBB postulates a pilot wave to explain experimental evidence.
Saying that dBB is 'wrong' is somewhat wild and unconsidered. The same wave-function is used to calculate the trajectories and the same predictions are made. I don't think you know enough about dBB to say these things.I still think it's wrong and somewhart contrived, but to relegate it [dBB] to an interpreation of the theory it rejects is probably unfair.
Mentz114 said:FrameDragger:
But SQM is saying that the pattern is determined by the wave-function otherwise there would be no interference pattern. SQM does not say that the particles behave like classical particles.
Saying that dBB is 'wrong' is somewhat wild and unconsidered. The same wave-function is used to calculate the trajectories and the same predictions are made. I don't think you know enough about dBB to say these things.
If you reject all this - do you think a Rubidium atom can somehow pass through both slits at the same time ?
Mentz114 said:Frame Dragger,
Fair enough. Quantum phenomena are certainly weird and trying to find intuitive meaning behind the equations is probably futile.
OK, but if the amplitudes are governed by a wave function, then there is path dependent phase, and so interference will take place when you sum the amplitudes from the different paths. This can only happen with waves, so a wave phenomenon is happening. You've just rephrased it in path integral terms.The amplitude for finding a particle in a state is the sum of the conditional amplitudes that it will land it that state given that it is in the possible previous states. If these amplitudes were real numbers rather than complex this would be a Markov process.
From this point of view, interference is not really a wave interference but rather a linear combination of conditional amplitudes. this is similar to a Markov process where the probability of finding a particle in a particular state is a sum of conditional probabilities.
Mentz114 said:OK, but if the amplitudes are governed by a wave function, then there is path dependent phase, and so interference will take place when you sum the amplitudes from the different paths. This can only happen with waves, so a wave phenomenon is happening. You've just rephrased it in path integral terms.
I don't know if we're talking about the same thing here. Solutions to the Schroedinger equation for realistic situations are always of the formI was trying to point out that this is really a diffusion process. Waves that satisfy the wave equation are not diffusion processes.
The wave function does not satisfy the wave equation but rather a complex heat equation. I guess you do get waves when you look at stationary solutions in the presence of potentials.
Mentz114 said:I don't know if we're talking about the same thing here. Solutions to the Schroedinger equation for realistic situations are always of the form
<br /> \psi(x,t)=Ae^{\frac{i}{\hbar}(Et+px)<br />
where E and p are the energy and momentum. This is a wave even for a free particle.
Mentz114 said:I don't know if we're talking about the same thing here. Solutions to the Schroedinger equation for realistic situations are always of the form
<br /> \psi(x,t)=Ae^{\frac{i}{\hbar}(Et+px)<br />
where E and p are the energy and momentum. This is a wave even for a free particle.
Mentz114 said:To be more precise, the plane-wave solution I quoted above won't be enough for most cases, but a linear combination of plane waves makes a nice wave-packet.
Just nit-picking ...
Frame Dragger said:Well, your question is at the heart of one of the major unsolved questions in modern physics. It was an interesting question, and bound to lead to some complex ruminations on the subject. And fireworks... musn't forget the fireworks lol.
mintparasol said:The lack of consensus is illuminating (pardon the pun!)
I had been under the impression that QM models were as immutable as, say, special relativity or the laws of thermodynamics
mintparasol said:I had been under the impression that QM models were as immutable as, say, special relativity or the laws of thermodynamics
DrChinese said:The mathematical formalism itself is essentially immutable (of course that could change) and has remained in place for over 80 years. What changes is the mapping of the formalism to underlying mechanical processes, something which is not strictly required for any theory. This "mapping" is the source of the debate and confusion, just in case that point was not clear from the above.
And by the way, there is a similar debate raging about relativity and its interpretations. Although the one about QM is more well known and tends to have more *robust* debate.
Frame Dragger said:No... you missed my point entirely. The experiment involving Rubidium showed a single atom having a unique wavefront just as a single photon does. The fact that it takes multiple passes (as you say, a buildup) to make the pattern visible is a limitation of our detection methods. If one could image a photon more exactly there would be a wavefront causing an interference pattern, visible or not. The dual nature of the quanta seems pretty clear. That's a limitation of the experimental apparaturs, but it's clear from the distribution... built over time as you say... that each individual photon, atom, etc, while observed at any given time to be particle or wave -like... has both properties at all times.
Frame Dragger said:To be fair to those scientists who stake their careers and reputations on various theories... it's easy to see politics stifling science in hindsight, but when your *** is on the line... not so easy. So, in some cases the debate is spirited for the sake of retaining one's viewpoint or standing, and sometimes it's spirited because the math says very strange things about the universe that we as humans do not see in our everyday lives (and recognize as such at least).
GR and SR have plenty of debate, including ideas such as treating time as separate from space. Einstein's theories however, have had the benefit of experiments which refute some counterclaims and support it. Time dilation, gravitational lensing, and more have been directly observed. By its very nature, QM defies that same degree of precision in the absence of new thinking, math, and technology.
Want to test GR? Make some really great telescopes and wait for the right time (or make some really good gyros and lasers in the extreme). Want to test SQM? Build the Large Hadron Collider and cross your fingers. You see the problem... ;)
mintparasol said:Ok, I've read some of the links posted here and have gleaned a little more understanding of what's going on here by some of your replies. I won't pretend to understand the math but think I have a better understanding of what's going on here in layman's terms.
Basically, as I see it, we see no evidence of the wave property of light from the firing of a single photon. We fire it thru the slits and it hits the detector screen and is detected at a point. We have no way of determining in advance where it will hit the detector screen. It is only after firing a whole lot of photons, either all at once, or one at a time, that the wave nature of light is revealed to us by means of an interference pattern at the detector.
This means to me at least, that we get a more meaningful view of the properties of light by considering the properties of many photons rather than the properties of a single photon.
It's interesting that the time factor (i.e. whether you fire the photons all at once or one at a time) makes no difference to the result of the experiment.
Frame Dragger said:You now understand the SQM interpreation of the experiment. I'd call the thread a rousing success! Differences in whether the experiment reveals the wave nature of light, or if it is the result of an ensemble, or pilot wave... you have the actual details of the mechanics down pat.
Finally, remember that if you CAN add an additional measuring device, it doesn't matter if you use the data or not. The fact that you COULD have by deploying more observation means that you can't see evidence of duality.
Yes, Maxwell's equations are the classical way. Light is waves.mintparasol said:This means to me at least, that we get a more meaningful view of the properties of light by considering the properties of many photons rather than the properties of a single photon.
Agreed. This is what led Feynman to say that the photon interferes with itself.mintparasol said:It's interesting that the time factor (i.e. whether you fire the photons all at once or one at a time) makes no difference to the result of the experiment..
mintparasol said:Hmmm, is it right to say then that we observe individual photons as particles and we find wave properties only when we measure the properties of many photons emanating from the same source. To me, this clears up the 'mystery' of duality completely
mintparasol said:Basically, as I see it, we see no evidence of the wave property of light from the firing of a single photon.
SimonA said:J12345 - are you attributing consciousness to particles? Bohr would just say that the measurement is the collapsing of the wave function, and that's the easy way out that physicists have followed for decades. You miss the subtle questions that we need to start asking again.