I want to understand positive operator valued measures in QM

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Discussion Overview

The discussion revolves around positive operator valued measures (POVMs) in quantum mechanics, particularly their role as observables and the underlying mathematical concepts such as the spectral theorem. Participants seek resources for understanding and clarify the definitions and implications of these measures.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants inquire about the meaning and implications of positive operator valued measures and their classification as observables.
  • Several references are suggested for further reading, including online resources and textbooks.
  • One participant argues that the outcomes of measurements associated with POVMs can be anything, emphasizing that the probabilities are determined by the density matrix.
  • Another participant defends the accuracy of the term "positive operator valued measure," linking it to properties of projector operators and spectral measures.
  • A counterpoint is raised regarding the completeness of projector valued measures (PVMs) in describing self-adjoint operators, noting that different operators can share the same PVM.
  • Participants discuss the relationship between bounded operators and their domains in the context of PVMs and spectra.

Areas of Agreement / Disagreement

There is no consensus on the completeness of PVMs in describing operators, with some participants asserting their limitations while others defend their utility. The discussion remains unresolved regarding the implications of POVMs versus traditional measurement interpretations.

Contextual Notes

Participants express varying levels of familiarity with functional analysis and measure theory, which may influence their interpretations and understanding of the concepts discussed. The discussion includes references to specific mathematical properties and theorems that are not fully explored.

Fredrik
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I want to understand positive operator valued measures in QM, in particular why they are considered "observables". Anyone know a good place to start reading about this?

I know some functional analysis and some measure theory, but I haven't made it all the way to the spectral theorem.
 
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Fredrik said:
I want to understand positive operator valued measures in QM, in particular why they are considered "observables". Anyone know a good place to start reading about this?

I know some functional analysis and some measure theory, but I haven't made it all the way to the spectral theorem.

Chapter 3 of
http://www.theory.caltech.edu/people/preskill/ph229/#lecture
 
Thank you. That looks like a good enough place to start.
 
What does "positive operator valued" or "projector valued" measure mean? Is this really an accurate naming?

I'm asking, because the possible outcomes in such measurements are still eigenvalues of a suitable operator, aren't they?
 
kith said:
What does "positive operator valued" or "projector valued" measure mean? Is this really an accurate naming?

I'm asking, because the possible outcomes in such measurements are still eigenvalues of a suitable operator, aren't they?

No. outcomes can be anything; the POVM only specifies their probabilities:
the probability the outcome associated with measurement of operator F_i occurs is
P_i = tr rho F_i, where rho is the density matrix of the measured system.
(from http://en.wikipedia.org/wiki/POVM )

This is far superior to the heavily idealizing Born interpretation, which claims that a measurement produces the exact eigenvalue of an operator, which is ridiculous whenever the eigenvalues of the operator in question are irrational numbers. (In particular, discrete spectra of all but the simplest Hamiltonians are irrational, but nobody is able to measure energies to infinitely many digits!)
 
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kith said:
What does "positive operator valued" or "projector valued" measure mean? Is this really an accurate naming?

Yes, it's accurate. First note that <projector operator> is a well defined concept in a Hilbert space. They are operators which have certain particular properties for which they are useful in quantum physics (2 one of them being boundedness and the property to be positively defined). Also <measure> is a concept used in Hilbert spaces through spectral measures for self-adjoint/unitary operators. So one achieves the most general description of self-adjoint operators through projector valued measures (PVM )by the spectral theorem of von Neumann. For positively defined operators, such as the statistical operator ρ of von Neumann, we also have POVMs as most people know them again through the spectral theorem. Actually, POVMs generalize PVMs in the sense discussed in https://wiki.physik.uni-muenchen.de/...8/87/POVMs.pdf page 4.
 
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dextercioby said:
So one achieves the most general description of self-adjoint operators through projector valued measures (PVM )by the spectral theorem of von Neumann.

Not quite. An operator contains more information than recorded in the PVM; therefore the latter gives not a full description of the operator, and hence not the most general one:

If A is a self-adjoint operator with discrete spectrum and not itself a projector then the operators
A and A^2 have different spectrum but the same associated PVM.
 
A good reference to start learning about the spectral theorem is Mathematical Physics by Robert Geroch, in the last few chapters of the book. He doesn't do the operator-valued measure approach, although he mentions it (I think it's still worth reading first, even if you are more interested in operator-valued measures). Very nice exposition, though.
 
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OK, I stand corrected. Nonetheless, A and A2 may not have the same domain...
 
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dextercioby said:
OK, I stand corrected. Nonetheless, A and A2 may not have the same domain...

They have the same domain iff A is bounded.

But A^2 and A^2+1 always have the same domain and the same PVM, but different spectrum.
 

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