Ballentine: Statistical Interpretation of QM

In summary, Ballentine believes that the statistical interpretation of QM is not conflicting with quantum theory and that it is possible to extend the formalism of QM by the introduction of joint probability distributions for position and momentum. He also states that the distinction between state preparation and measurement is important.
  • #1
strangerep
Science Advisor
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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
[itex]|\psi(\mathbf{r})|^2[/itex] 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".
 
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  • #2
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.
 
  • #3
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. :-)
 
  • #4
Sorry for the tricky question. As far as I can tell, the only non-controversial answer could be: "I don't know".

Eugene.
 

1. What is "Ballentine: Statistical Interpretation of QM"?

"Ballentine: Statistical Interpretation of QM" is a book written by physicist and professor of physics at the University of Amsterdam, Leslie E. Ballentine. It is a comprehensive guide to the statistical interpretation of quantum mechanics, providing a detailed analysis of the mathematical foundations and implications of this interpretation.

2. What is the statistical interpretation of quantum mechanics?

The statistical interpretation of quantum mechanics is an interpretation of quantum theory that explains the probabilistic nature of quantum measurements. It states that the outcomes of quantum measurements are inherently random and can only be described by probabilities.

3. Who is Leslie E. Ballentine?

Leslie E. Ballentine is a renowned physicist and professor of physics at the University of Amsterdam. He is known for his contributions to the field of quantum mechanics, particularly his work on the statistical interpretation of quantum mechanics.

4. What are the mathematical foundations of the statistical interpretation of quantum mechanics?

The statistical interpretation of quantum mechanics is based on the mathematical framework of Hilbert space and the measurement postulate of quantum mechanics. It also involves the use of complex numbers and linear operators to describe the behavior of quantum systems.

5. What are the implications of the statistical interpretation of quantum mechanics?

The statistical interpretation of quantum mechanics has several implications, including the idea that the behavior of quantum systems is inherently probabilistic, the existence of quantum superposition, and the role of measurement in collapsing the wave function. It also raises questions about the nature of reality and the relationship between the observer and the observed in quantum systems.

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