Ballentine: Statistical Interpretation of QM

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Discussion Overview

The discussion revolves around the statistical interpretation of quantum mechanics as presented by L.E. Ballentine, particularly focusing on the implications of this interpretation in relation to particle behavior, measurement, and the double-slit experiment. Participants explore the nuances of Ballentine's arguments and their relevance to contemporary understandings of quantum theory.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants reference Ballentine's assertion that a particle can be considered to have definite but unknown values of position and momentum, suggesting a statistical interpretation of quantum mechanics.
  • There is a discussion about the distinction between state preparation and measurement, with emphasis on the minimum dispersion principle as outlined by Ballentine.
  • One participant questions how Ballentine's interpretation aligns with experimental results from the past two decades, suggesting that the ensemble interpretation might still be consistent with new findings.
  • Another participant raises the classic double-slit experiment, questioning whether a single electron passes through one or both slits, highlighting the ambiguity in interpreting particle behavior under the statistical framework.
  • There is a mention of a potential conflict between Ballentine's use of the term "particle" and the interpretation of quantum mechanics that emphasizes fields, indicating a need for further exploration of these concepts.
  • One participant humorously acknowledges the complexity of the question regarding the double-slit experiment, suggesting that a non-controversial answer might simply be "I don't know."

Areas of Agreement / Disagreement

Participants express differing views on the clarity and implications of the statistical interpretation, particularly in relation to the behavior of particles in quantum mechanics. There is no consensus on how to interpret the results of the double-slit experiment or the implications of Ballentine's framework.

Contextual Notes

The discussion highlights limitations in understanding the statistical interpretation, particularly regarding the definitions of "particle" and the implications of measurement versus state preparation. Participants note the unresolved nature of these concepts in the context of quantum mechanics.

strangerep
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This is a continuation of discussions from another thread:

https://www.physicsforums.com/showthread.php?t=490677&page=2

I believe it deserves its own thread instead of hijacking the other one.

"Ref 3" in what follows is this paper:

L.E. Ballentine, "The Statistical Interpretation of QM",
Rev Mod Phys, vol 42, no 4, 1970, p358.

Fredrik said:
[...] on p. 361 of ref. [3], [Ballentine] says, the Statistical
Interpretation considers a particle to always be at some position in
space, each position being realized with relative frequency
|\psi(\mathbf{r})|^2 in an ensemble of similarly prepared
experiments. Later [3, p. 379] he states, there is no conflict with
quantum theory in thinking of a particle as having definite (but, in
general, unknown) values of both position and momentum.

It's easy to get a misleading impression by quoting bits out of context.

The context of Ballentine's remark on p379 is that "it is possible to
extend the formalism of QM by the introduction of joint probability
distributions
for position and momentum (section 5 of his paper).
This demonstrates that there is no conflict with quantum theory in
thinking of a particle as having definite (but, in general, unknown)
values of both position and momentum."

It's also essential to understand Ballentine's points about the
distinction between state preparation and measurement. See p365,366.
"The statistical dispersion principle which follows from QM formalism
is a statement about the minimum dispersion possible in any state
preparation. This is distinct from errors of simultaneous measurements
of q and p one one system." This argument should be understood
in the context of Ballentine's discussion of his Fig 3.

unusualname said:
I'm not sure how Ballentine's thinking has
developed with the huge number of sophisticated experimental results in
the last 20 years, but perhaps it is possible to make the ensemble
interpretation consistent with everything so far discovered, since it
doesn't say much beyond the basic mathematical model of QM. But it's
terribly dull ;-)

If "dull" means no accompanying fairy stories, then I'm ok with that. :-)

unusualname said:
Do you really think the correct (and simplest) theory of QG will still rely on
a vague "interpretation"?

The only thing I can say with confidence about this is that the "correct"
theory of QG will not contradict experimental results. :-)

But you're kinda putting words in my mouth. I don't think the statistical
interpretation is "vague".
 
Last edited:
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strangerep,

what you (and Ballentine) would say about a single electron passing through the double-slit setup. Does this electron pass through one slit? Or through two slits at once?

Eugene.
 
meopemuk said:
what you (and Ballentine) would say about a single electron passing through the double-slit setup. Does this electron pass through one slit? Or through two slits at once?

I thought you might bring that up! :-)

I can't say what Prof Ballentine would say, since I don't have the necessary
telepathic link.

One of the (other) reasons for starting this thread is that Ballentine still speaks
in terms of "particles", though in a strictly statistical context. In such a context,
your question is unanswerable (imho) because it presumes more than the
theory contains.

Also, I had intended to pursue some of this in parallel with Arnold's thread
over on Independent Research forum -- since it's not entirely clear to me
where the overlap between Ballentine's statistical interpretation and his use
of the word "particle", and Arnold's interpretation with emphasis on fields, starts
and ends.

Interestingly, I just noticed that Ballentine mentions a quote of Mott about how
"students shouldn't be taught that [...elementary particles...] are not particles",
which seems to be at odds with the picture that Mott himself portrayed in his
alpha particle track analysis paper which we discussed in other threads.
But I need to read a bit more of both to form a better view about that.
Maybe I'll bring it up in Arnold's thread -- later. :-)
 
Sorry for the tricky question. As far as I can tell, the only non-controversial answer could be: "I don't know".

Eugene.
 

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