A Why Unitary Evolution? QM Justification Ideas

  • #51
Got the e-book. Just skimming now. I love the remark: 'To top it all, I was buried by the worst advice I ever received, to learn the topic from Dirac’s book itself!'

It was the second serious book on QM I read and know the issue only too well. The first was Von Neumann's book which is excellent for mathematicians since it is just an extension of Hilbert-Space theory. I was confident when I went on to Dirac but became unstuck with that damnable Dirac Delta function. It led me on a sojourn in Rigged Hilbert Spaces that had nothing to do with physics. I came out the other end with the issues resolved - but at that stage of my QM journey, it was not a good move.

Thanks
Bill
 
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  • #52
But Dirac's book is excellent. What's the problem with it? Von Neumann is of course mathematically rigorous and Dirac is not.
 
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  • #53
vanhees71 said:
But Dirac's book is excellent. What's the problem with it? Von Neumann is of course mathematically rigorous and Dirac is not.

It is excellent, physically better Von-Neumann. The only issue, which has been 'fixed' and is no longer of any relevance, is the diatribe Von Neumann writes about it at the beginning of his book. It is easy for a math graduate to read Von Neumann after studying Hilbert Spaces, but Dirac is more problematic. I personally believe every math degree should include distribution theory because of its wide use in applied math. As part of that, a few paragraphs like that found in Ballentine is all that is needed. I am going through Talagrand's book and it has a more complete explanation. If that was done first, then Dirac is fine. Perhaps include it in a modern preface to both books - just an idea.

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Bill
 
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  • #54
vanhees71 said:
Note that, despite for claims often to be read in textbooks, there's no need for parity or time-reversal symmetry for the detailed-balance relations to be valid.
Interesting, can you give a reference with more details?
 
  • #57
vanhees71 said:
But Dirac's book is excellent. What's the problem with it?
It has an explicit collapse postulate!
 
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  • #58
If that were a problem, you couldn't recommend very many otherwise excellent QT textbooks. Indeed, physics students also have to learn to "not listen to their words but looking at their deeds" (as Einstein adviced concerning all writings of theoretical physicists). That the collapse postulate is at best superfluous and at worst simply a contradiction to causality in the relativistic context should be obvious (though obviously it isn't for many philosophy-inclined physicists who still think that it's needed), but all this is off-topic here in the scientific part of the QT forum!
 
  • #59
vanhees71 said:
physics students also have to learn to "not listen to their words but looking at their deeds" (as Einstein adviced concerning all writings of theoretical physicists).
This also applies to reading your lecture notes and your contributions to PF.. The collapse - not necessarily the von Neumann form but in the general POVM related version - is used informally almost everywhere, namely whenever one argues how a state is prepared.
 
  • #60
For sure, it's not an instantaneous collapse affecting the physics at all points in space simultaneously. All our experiments are local, and nothing can violate the relativistic speed limit of signal propagation.
 
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  • #61
A. Neumaier said:
It has an explicit collapse postulate!
It does not. And not because Dirac uses the word "principle" instead of "postulate", or the word "jump" instead of "collapse". But this is indeed off-topic.
 
  • #63
A. Neumaier said:
Again, this is off-topic, but: thank you, I actually have read Dirac, both the original and the first Russian edition edited by Fock. Nowhere in the book did he elevate the notion of throwing out a part of the probability distribution describing a physical system to a grand status of a physical principle (using Dirac's language when writing the book). Therefore, not even esteemed Peres could find (not that he would or should have) even a small section in Dirac's book with the words "jump" and "principle" in its title (Dirac never uses the word "collapse" in his book). However, you will find an entire chapter on "The Principle of the Superposition" and separate sections on "Heisenberg's Principle of Uncertainty" and "The Action Principle".
 
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  • #64
physicsworks said:
Again, this is off-topic, but: thank you, I actually have read Dirac, both the original and the first Russian edition edited by Fock. Nowhere in the book did he elevate the notion of throwing out a part of the probability distribution describing a physical system to a grand status of a physical principle (using Dirac's language when writing the book).
I have just now re-read the relevant section of Dirac's book (The Principles of Quantum Mechanics, 1982 ed). On p35 he writes:

Dirac said:
We now make some assumptions for the physical interpretation of the theory. If the dynamical system is in an eigenstate of a real dynamical variable ##\xi##, belonging to the eigenvalue ##\xi'##, then a measurement of ##\xi## will certainly give as result the number ##\xi'##. [...]
This is not exactly the usual collapse-like assumption, but Dirac goes on with: "some of the immediate consequences of the assumptions will be noted ..." (my emboldening). Among these "consequences of the assumptions" is the passage referenced by Peres and Terno, i.e., (p36):
Dirac said:
When we measure a real dynamical variable ##\xi##, the disturbance involved in the act of measurement causes a jump in the state of the dynamical system. 'From physical continuity, if we make a second measurement of the same dynamical variable ##\xi## immediately after the first, the result of the second measurement must be the same as
that of the first. Thus after the first measurement has been made, there is no indeterminacy in the result of the second. Hence, after the first measurement has been made, the system is in an eigenstate of the dynamical variable ##\xi##) the eigenvalue it belongs to being equal to the result of the first measurement. This conclusion must still hold if the second measurement is not actually made. In this way we see that a measurement always causes the system to jump into an eigenstate of the dynamical variable that is being measured, the eigenvalue this eigenstate belongs to being equal to the result of the measurement.
It's pretty clear that Dirac infers a jump in the state of system (what in modern times would normally be called "collapse") as an "immediate consequence" of his assumption. Sure, it's not in a section title, afaict, but so what?
 
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