Bell violation with extra particles

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Discussion Overview

The discussion revolves around the implications of measuring spin in quantum mechanics, particularly in the context of Bell's theorem and the behavior of particles in a Stern-Gerlach experiment. Participants explore the differences between classical and quantum models of spin measurement, the detection of particles, and the potential for extra particles in the experimental setup.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that when measuring spin at 90 degrees, particles may not definitively go up or down, leading to a hypothesis that particles close to this angle tumble and do not reach the detector.
  • Others argue that the classical model fails to account for the observed correlations in spin measurements, suggesting that missing particles could explain discrepancies between classical and quantum predictions.
  • A later reply questions the existence of tumbling or momentum loss effects, asserting that experiments show 100% matching results regardless of the orientation of the measuring devices.
  • Some participants reference experimental results that demonstrate violations of Bell's inequality, indicating that high detection efficiency can eliminate detection loopholes.

Areas of Agreement / Disagreement

Participants express differing views on the behavior of particles near 90 degrees and the implications for quantum mechanics versus classical interpretations. There is no consensus on the existence of tumbling effects or the implications of detection efficiency in relation to Bell's theorem.

Contextual Notes

The discussion includes unresolved assumptions about the behavior of particles in magnetic fields and the conditions under which measurements are made, as well as the implications of detection efficiency on the outcomes of experiments.

edguy99
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Taken from an earlier thread:

"If the two devices are aligned in matching orientations (in opposite directions to allow for the initial state), then QM says that 100% of the results should match. If either of the two devices is turned at 90 degrees to the original orientation, then QM says that the average correlation should be zero, so 50% of the results should match and 50% should be different. If either device is turned to 45 degrees from the original orientation, then the classical projection of one direction on the other is cos 45 degrees, which is about 0.7 (70%), so to get this correlation we need 85% of results to be the same and 15% to be different."

Wrt to the style of measurement shown http://www.upscale.utoronto.ca/PVB/Harrison/SternGerlach/SternGerlach.html" the spinning sphere can model the up and down motion but fails the Bell test to predict the correct percent of same or different spin orientations that two observers see.

One problem with the classical model is the measurement of spin at exactly 90 degrees. Should the particle go up or down? One way to resolve this is: any particle measured that is within 12.5 degrees of 90 degrees to the measuring device, will not go up or down but will start to tumble in the magnetic field with loss of momentum. These particles do not make it to the detector.
clock45_p1.jpg


So we setup the experiment with Bob and Alice offset by 45 degrees:
clock45_p2.jpg


This setup does meet the test of the observed 15% difference, but does anyone know if these devices end up with extra particles in them and if there is any kind of relationship between the spin offset and/or the extra particles left behind?
 
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edguy99 said:
... One problem with the classical model is the measurement of spin at exactly 90 degrees. Should the particle go up or down? One way to resolve this is: any particle measured that is within 12.5 degrees of 90 degrees to the measuring device, will not go up or down but will start to tumble in the magnetic field with loss of momentum. These particles do not make it to the detector.

...

I think you are trying to say that not all particles are detected, and that the missing particles account for the difference between a classical model of spin and the quantum model. Or?

I am trying to narrow down what you are hypothesizing.
 
DrChinese said:
I think you are trying to say that not all particles are detected, and that the missing particles account for the difference between a classical model of spin and the quantum model. Or?

I am trying to narrow down what you are hypothesizing.

Basically yes. In this model of a spin 1/2 particle, all particles do not reach the detector, specifically particles that are close to 90 degrees to the measuring device (or their motion is so disrupted by the tumbling that their spin direction would have to be considered random even if they happen to hit the detector).
 
edguy99 said:
Basically yes. In this model of a spin 1/2 particle, all particles do not reach the detector, specifically particles that are close to 90 degrees to the measuring device (or their motion is so disrupted by the tumbling that their spin direction would have to be considered random even if they happen to hit the detector).

Well, there is no such observed effects as tumbling or momentum loss due to spin. Further, the experiment is rotationally invariant. You will see 100% matching regardless of how you orient the SG apparatus - 0, 45, 90 degrees, no matter, same result. The effects you hypothesize would be easily seen in basic experiments, and they just don't happen.

Further, all of this is supported by experiments with many different kinds of particles, including light. In addition, there have been tests in which 100% of all pairs are detected and they show the same result.
 
DrChinese said:
.. In addition, there have been tests in which 100% of all pairs are detected and they show the same result.

Thanks, appreciate a link on this.
 
edguy99 said:
Thanks, appreciate a link on this.

Sure:

http://www.nature.com/nature/journal/v409/n6822/full/409791a0.html

"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."
 

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