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Is quantum mechanics a complete theory of nature? |
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| Mar9-12, 10:40 AM | #18 |
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Is quantum mechanics a complete theory of nature? |
| Mar10-12, 12:36 AM | #19 |
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There are 8 pages of historical developments and experimental discussions in the paper you cite but only two sentences are used to define what a “single photon” is. I don't question the accuracy of the experiments or that they are able to make good predictions. I question the assumptions that they begin with and the logic behind them. Can you cite something more basic? I believe that the Marshall and Santos papers I cited do a better job of looking at fundamentals. Although they do not offer a more accurate theory they have the advantage that they reject non-locality. Will you comment on their argument that when the zero point field is used to describe the photon it is actually a classical model? |
| Mar11-12, 01:41 AM | #20 |
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But then I do not understand how this bunching model is better. Or maybe I do: Well, I do not agree. Single-photon model by itself does not conflict with local realism. On the other hand Bell theorem applies to your bunching model just as well. |
| Mar11-12, 04:30 AM | #21 |
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So, how can your OP possibly ever be definitively answered? |
| Mar12-12, 01:04 PM | #22 |
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“The one-photon state has the important and distinctive property that it can produce only a single current pulse in the ionization of a photodetector.” DrChinese, If we are talking about one-photon states then when you said Loudon also states the following: “A one-photon excitation in such a mode (spatial mode) is distributed over the entire interferometer, including both internal paths.” page 2. I understand this to mean that the one-photon state is delocalized and because it is in both arms at the same time it is a non-local definition. It should not be surprising that a non-local model would result in non-locality. When quantum mechanics rejects a physical model such as bunching because it is viewed as incomplete they insist that a better model must give better predictions. IOW better predictions is more important than a local theory? We can have both locality and predictive power if we admit that it is impossible to know for sure what constitutes a detection event. ThomasT do you equate reality with what we observe? IOW is there more to reality than what we observe? |
| Mar12-12, 01:52 PM | #23 |
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As to the bunching phenomena you postulate, all you have to do is give me a specific scenario and I believe we can explain why this does not apply. Please recall that there are probably hundreds of different types of Bell tests which violate local realism, many which do not use photons at all. For example, see: http://www.nature.com/nature/journal.../409791a0.html Local realism is the idea that objects have definite properties whether or not they are measured, and that measurements of these properties are not affected by events taking place sufficiently far away1. Einstein, Podolsky and Rosen2 used these reasonable assumptions to conclude that quantum mechanics is incomplete. Starting in 1965, Bell and others constructed mathematical inequalities whereby experimental tests could distinguish between quantum mechanics and local realistic theories. Many experiments have since been done that are consistent with quantum mechanics and inconsistent with local realism. But these conclusions remain the subject of considerable interest and debate, and experiments are still being refined to overcome ‘loopholes’ that might allow a local realistic interpretation. Here we have measured correlations in the classical properties of massive entangled particles (9Be+ ions): these correlations violate a form of Bell's inequality. Our measured value of the appropriate Bell's ‘signal’ is 2.25 ± 0.03, whereas a value of 2 is the maximum allowed by local realistic theories of nature. In contrast to previous measurements with massive particles, this violation of Bell's inequality was obtained by use of a complete set of measurements. Moreover, the high detection efficiency of our apparatus eliminates the so-called ‘detection’ loophole. So your model needs a little revving up to explain this. 'Cause there ain't no bunching of Beryllium.
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| Mar13-12, 12:49 AM | #24 |
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| Mar14-12, 11:24 AM | #25 |
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Photons are localized with a diffuse external field and a single frequency. By themselves they do not have sufficient energy to cause a detection event, but the superposition of fields of many photons leads to intensities sufficient to cause a detection event. Detections are caused by the superposed fields of photons. |
| Mar14-12, 12:36 PM | #26 |
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2. No, it's not presumptuous in light of Bell. If you accept "elements of reality" as defined by EPR, you must reject local realism. Or not, if you simply reject everything you don't want to believe. (I can't assist on that side.) |
| Mar14-12, 12:41 PM | #27 |
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A better model is a better model. However, we now know that won't be one which is local realistic. |
| Mar14-12, 02:25 PM | #28 |
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2.From my post #4 The only reason you know that there will be no local realistic model is because it was defined to be non-local. |
| Mar14-12, 02:27 PM | #29 |
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Recognitions:
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Important things first:
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| Mar14-12, 03:14 PM | #30 |
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![]() I thought the citation might help nortonian, but he would have to read it first. |
| Mar16-12, 12:19 AM | #31 |
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All one has to do is demonstrate that falsifiable prediction of theory actually fails. Question for you: is quantum entanglement falsifiable prediction of quantum mechanics? |
| Mar16-12, 04:55 AM | #32 |
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Another fundamental question concerns how qm deals with time. In optical experiments qm uses a single time parameter, the phase, when defining photons. A model that uses superposed photons to define detection is able to include continuous time into the energy absorption/emission process. The fields of superposed photons cause the outer electrons of photosensitive atoms to oscillate. If the superposition is of sufficient intensity the electron is forced into a higher orbital, where after a finite decay time it drops back and emits a photon. The conservation of momentum is exactly obeyed. In the qm model the superposed fields and detection event are both included in the photon so that observation is an instantaneous event. (The path integral method does use both times but it integrates over all time a questionable practice.) The interaction does not take place in continuous time as would be necessary to include momentum in a description. If we introduce momentum into a description of photon states, how does a single photon cause excitation? It would be necessary for the photon to impact the electron with precisely the amount of energy to raise it into a higher orbital without knocking it out of the atom completely. Visualization is not possible. I have a problem with that because I am thinking, what are they hiding? Where is the momentum? The important stuff, the fundamentals, the details are skipped over. Quantum mechanics treats time and momentum inconsistently. |
| Mar16-12, 06:13 AM | #33 |
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Recognitions:
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| Mar16-12, 11:56 AM | #34 |
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Then the difference is that we can not be sure that detection events will pair up perfectly with assumed perfect detectors. Basically we can not claim that fair sampling assumption holds and therefore Bell theorem does not apply. However if detection events would pair up perfectly for efficient detection then there is no difference. |
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