Jaynes on probability in quantum theory

In summary: The only part about the ZPE is the one in the introduction and the one in section 6.5. The rest of the paper is about Jaynes' Bayesian approach to quantum mechanics, which is not widely accepted in the scientific community. Overall, the paper is more of a philosophical discussion rather than a scientific one.
  • #1
A. Neumaier
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This was off-topic in the thread on vacuum fluctuations where the quote appeared, so I opened a new one.

ftr said:
Arnold, I found this paper(researching a different subject) by Jaynes which you mention his name in context of entropy issues in FAQ. But This paper has some relevance to the discussion, what do you think(I kind like what he is saying, but I need to study it more)

http://bayes.wustl.edu/etj/articles/prob.in.qm.pdf

I didn't know the paper before, so first need to read it...
 
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  • #2
I have a question on equation 30 of this paper. I too am studying this paper but need clarity.

Is the usage of [tex]\Gamma [/tex] the effective action as per Weinberg's treatment

https://arxiv.org/abs/hep-th/0507214

as opposed to the christoffel connection coefficient?

Or is the two technically one and the same?
 
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  • #3
Thanks for opening the thread. The talk about the ZPE I thought is well connected to vacuum, but the article seems to tie many issues in QM/QFT in general. I hope I can have more questions soon.
 
  • #4
ftr said:
The talk about the ZPE I thought is well connected to vacuum, but the article seems to tie many issues in QM/QFT in general.
The main goal of the article, as stated in the abstract, is something quite different:
Jaynes said:
we explore the consequences of the unied view, that all probability signifies only incomplete human information.
Jaynes effectively claims that quantum physics is not about properties of Nature but about human knowledge management. I find his Bayesian, subjective probability view untenable as a basis for objective physics. The last two sections of Chapter 10 of my online book give a specific critique of his views in the context of statistical mechanics (where its strength is supposed to lie).

According to the abstract, his main critique to which he targets his exploration is
Jaynes said:
probabilities calculated within a pure state have a different character than the probabilities with which different pure states appear in a mixture, or density matrix. [...] this viewpoint leads to so many paradoxes and mysteries
though in the main text he doesn't even state what he means by this, let alone explain the content of the paradoxes and mysteries. This already shows that something is seriously wrong with the paper - it is a sequence of loosely related philosophical musings, not a proper scientific paper. (He has no qualms to talk on p.3 about the problem of generating infinities caused by using ##\infty^2## more degrees of freedom than the infinitely many degrees of freedom actually used by Nature, though ##\infty^2## times ##\infty## is still ##\infty##, as we know since Cantor.)

But I agree with this critique, and think that one cannot reasonably uphold the view that the use of density matrices in quantum physics (for Lindblad's equation or statistical mechanics) should be interpreted as due to a lack of information about the true, pure state. They contain the complete information that can be possibly obtained about the state. Once this is acknowledged, most problems associated with wave functions go away, when combined with another remark by Jaynes, on p.11:
Jaynes said:
in basic probability theory, ##\Delta F## represents fundamentally the accuracy with which we are able to predict the value of ##F##. This does not deny that it may be also the variability seen in repeated measurements of ##F##; but the point is that they need not be the same
My thermal interpretation makes this self-evident observation the basis of a common sense interpretation of quantum mechanics, without giving up objectivity or introducing human elements into the foundations.

A problem with Jaynes' arguments is that he bases much on arguments of authority from sources now mostly 50 or more years old (hence were already 30 or more years old when he wrote the paper). That he takes Bayesian computational results on p. 8 as support for Bayesian philosophy (although algorithms are immune to philosophy since all Bayesian statistics has a frequentist interpretation) is also strange.

ftr said:
The talk about the ZPE I thought is well connected to vacuum, but the article seems to tie many issues in QM/QFT in general.
He repeats well-known stuff summarized in his statement on p.11:
Jaynes said:
(1) the experimental facts do not require vacuum fluctuations to be real events
and adds (in my opinion without further gain in insight) his own subjective philosophy.

I argue in my Insight articles (and in the discussions of them) far more strongly that vacuum fluctuations cannot be real events since they lack all dynamic characteristica that go with real events.

Thus to answer your query, you can look at the section on the zero-point energy as a superficial and mostly historical discussion of some pros and cons of the two sides of the debate, and you can take the paragraph before this section and the conclusion of the paper as indication that he takes in this debate the same side as I, though for completely different reasons.
 
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  • #5
To answer the question concerning Eq. (30). Here ##\Gamma## is the width of the Lorentzian. It's easy to show by using a contour integral in the complex energy (freuquency) plain to get the Fourier transform to the time domain. It shows that ##\Gamma=1/\tau## is the inverse lifetime of the harmonic excitation described by the Lorentzian. Obviously ##\tau## is the time over which the amplitude of the oscillation decreases by a factor of ##\mathrm{e} \simeq 2.71828##.
 
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  • #6
Thanks Vanhees71
 
  • #7
A. Neumaier said:
The main goal of the article, as stated in the abstract, is something quite different:

well, this is the last sentence in the abstract.

"We examine in detail only one of the issues this raises: the reality of zero-point energy."

But thanks for the overall explanation. However, I was more interested in his idea of oscillators coupling, I am still studying it.
 
  • #8
ftr said:
"We examine in detail only one of the issues this raises: the reality of zero-point energy."
But the other items were not really examined at all.
 

Related to Jaynes on probability in quantum theory

1. What is Jaynes' theory on probability in quantum theory?

Jaynes' theory, also known as the MaxEnt approach, states that the probability of a given event in quantum theory can be determined by maximizing the entropy of the system subject to the constraints of the available information.

2. How does Jaynes' theory differ from the traditional approach to probability in quantum theory?

The traditional approach to probability in quantum theory, known as the Born rule, assigns probabilities based on the square of the wave function. Jaynes' theory, on the other hand, takes into account all available information and does not rely on the wave function.

3. What are the advantages of using Jaynes' theory in quantum theory?

Jaynes' theory allows for a more consistent and objective way to assign probabilities in quantum theory, taking into account all available information rather than just the wave function. It also allows for the incorporation of prior knowledge and can lead to more accurate predictions.

4. Are there any limitations to Jaynes' theory in quantum theory?

One limitation of Jaynes' theory is that it may not be applicable in cases where there is limited or conflicting information available. It also does not provide a physical interpretation of the wave function, which is a key concept in quantum theory.

5. How has Jaynes' theory been received in the scientific community?

Jaynes' theory has been met with both praise and criticism in the scientific community. While some have embraced it as a more principled approach to probability in quantum theory, others argue that it is incomplete and does not fully explain the behavior of quantum systems.

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