The Myth of Wave-Particle Duality

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SUMMARY

The discussion centers on the interpretation of wave-particle duality in quantum mechanics, particularly referencing Ballentine's 1970 work, "The Statistical Interpretation of Quantum Mechanics." Ballentine argues that the wave function represents an ensemble of particles rather than individual particles, challenging the notion of wave-like behavior as an inherent property of particles. Participants debate the implications of this view, questioning the validity of experiments that demonstrate wave behavior and emphasizing the role of statistical interpretations in quantum mechanics. Key figures mentioned include Duane, Lande, and Mott, highlighting the historical context of these interpretations.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly wave functions and probability waves.
  • Familiarity with the historical context of quantum theory, including contributions from Duane and Lande.
  • Knowledge of statistical mechanics and its application in quantum interpretations.
  • Awareness of the philosophical implications of quantum mechanics interpretations, such as Many-Worlds Interpretation (MWI).
NEXT STEPS
  • Research the implications of the de Broglie wavelength on electron behavior in atomic orbitals.
  • Explore the concept of Bose-Einstein condensation and its relation to quantum particles.
  • Investigate the role of measurement in quantum mechanics and its effect on particle-wave interpretations.
  • Examine the historical debates surrounding wave-particle duality and the interpretations of quantum mechanics.
USEFUL FOR

Quantum physicists, students of quantum mechanics, philosophers of science, and anyone interested in the foundational debates surrounding wave-particle duality and its interpretations.

  • #61
SpectraCat said:
I think that what I should have said above is that the statistical interpretation requires EITHER local hidden variables, OR it requires superluminal hidden variables. I guess this is what Demystifier meant when he described Bohmian mechanics as a specific realization of the statistical interpretation, because BM requires the quantum potential (or equivalent) which takes care of the superluminal stuff. Is that correct?
Yes, I would agree with that. And from the Ballentines textbook, it seems that he finds nonlocal hidden variables to be a more viable option.

It's also interesting to see what he says about the Bohmian interpretation (in the same textbook):
"The most important consequence of Bohm's theory is its demonstration that, contrary to previous belief, it is logically possible to give a more detailed account of microscopic phenomena than that given by the statistical quantum theory. The significance and utility of the resulting quantal trajectories, however, remain controversial."
 
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  • #62
Demystifier said:
That's not quite correct. The Bohmian approach needs only ONE of these two assumptions, because they are equivalent. And not for each particle separately, but for all particles at once.

Quantum Potential and the Bohm Omniscient Wave Function (BOWF) is equivalent? I thought BOWF is pure information only while the Quantum Potential is some kind of force that pushes the particle to either pass thru the left or right slit depending on how the BOWF able to detect configuration changes even a billion light years away.

I read in a book someone asking how a particle can be pushed. Some suggest a electron may have an internal part and there may be some kind of nano-jetpack that can manuever it. Lol... So how can the particle be influenced to take the left or right slit? Don't say initial condition, take a case where a quantum potential can influence it.. what's a good example?






Well, I like to view the Bohmian interpretation as a concrete realization of the more general Ballentine interpretation.
 
  • #63
Varon said:
So how can the particle be influenced to take the left or right slit? Don't say initial condition, take a case where a quantum potential can influence it.. what's a good example?
To say "initial condition" is not in contradiction with saying that it is influenced by the quantum potential. Both answers are correct, so it's not clear to me what kind of an answer do you actually want. :confused:

Or consider a CLASSICAL particle. What will determine the slit through which the particle will pass? Initial position? Classical force derived from a classical potential? Isn't it obvious that both answers are correct?
 
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  • #64
Demystifier said:
To say "initial condition" is not in contradiction with saying that it is influenced by the quantum potential. Both answers are correct, so it's not clear to me what kind of an answer do you actually want. :confused:

Or consider a CLASSICAL particle. What will determine the slit through which the particle will pass? Initial position? Classical force derived from a classical potential? Isn't it obvious that both answers are correct?

I thought that in the concept of quantum potential. Even if the initial condition is equal.. meaning the particle is sent off from the emitter straight. The quantum potential can push the particle while in mid flight.. this is why they mentioned it in the book (I forgot the title) how the electron may have structure that allows this propulsion system.
 
  • #65
Varon said:
Even if the initial condition is equal.. The quantum potential can push the particle while in mid flight..
What you suggest here may be achieved with a time dependent quantum potential, provided that two particles are fired at different times. However, in a typical 2-slit experiment the quantum potential is usually time-independent to a great accuracy.
 

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