Why Unitary Evolution? QM Justification Ideas

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Discussion Overview

The discussion revolves around the justification for the unitary evolution of physical systems in quantum mechanics, particularly in the context of teaching non-relativistic quantum mechanics. Participants explore various arguments and perspectives regarding why unitary evolution is favored over more general completely positive trace-preserving (CPTP) maps.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Homework-related

Main Points Raised

  • Some participants note that the usual justification for unitary evolution involves arguments related to probability conservation, which could also apply to CPTP maps.
  • One participant suggests that a symmetry approach, particularly through group theory, may provide a plausible heuristic for understanding unitary evolution in relation to the Galilei group and Newtonian spacetime.
  • Another participant raises a concern that energy conservation might not hold in non-unitary evolution, citing eigenvalues that could be less than or greater than one.
  • Some participants argue that while unitarity is mathematically appealing and preserves probabilities, it may not encompass the entirety of the story, especially when considering curved spacetimes in general relativity.
  • A later reply introduces the idea that the evolution of systems in cosmological contexts, such as deSitter space, may challenge the notion of fundamental unitarity.

Areas of Agreement / Disagreement

Participants express a range of views on the justification for unitary evolution versus CPTP maps, indicating that multiple competing perspectives remain. The discussion does not reach a consensus on the fundamental nature of quantum evolution.

Contextual Notes

Participants acknowledge the complexity of the topic, noting limitations in applying certain mathematical frameworks to introductory teaching and the challenges posed by transitioning from classical to quantum mechanics.

Who May Find This Useful

This discussion may be of interest to educators in quantum mechanics, researchers exploring foundational questions in quantum theory, and students seeking to understand the implications of unitary versus non-unitary evolution in quantum systems.

  • #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.
 
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  • #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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