A Fundamental Theorem of Quantum Measurements

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The Fundamental Theorem of Quantum Measurements states that a set of operators satisfying a specific condition can describe measurements with discrete outcomes. When considering continuous measurement outcomes, the probability density replaces the probability, leading to integrals over subsets to calculate probabilities. The discussion highlights the mathematical correctness of using these integrals but questions the physical existence of continuous observables, suggesting that measurement outcomes are inherently discrete. The conversation also emphasizes that while continuous observables exist mathematically, their physical representation in experiments may not align with this idealization. Overall, the debate centers on the interpretation of quantum measurements and the nature of observables in quantum mechanics.
  • #61
bhobba said:
Get your issue now - yes that's right. But I don't think those into mathematical modelling as a discipline are that unconcerned about experimental verification of their models :smile::smile::smile::smile::smile::smile::smile:

Thanks
Bill
If what you mean by "unconcerned" is concerned, then that certainly seems to be the case for string theorists.
 
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  • #63
bhobba said:
We are getting off topic here, but IMHO, and the opinion of others, for what you said, and other reasons, string theory has morphed a bit:
https://www.quantamagazine.org/string-theorys-strange-second-life-20160915/

THanks
Bill
Rather than saying we are getting off topic, why not say the topic is evolving/morphing in interesting ways?
That was a fun article, thanks, but not much about experimental confirmation of string theory.

From the article: "Using the physical intuition offered by strings, physicists produced a powerful formula for getting the answer to the embedded sphere question, and much more. “They got at these formulas using tools that mathematicians don’t allow,” Córdova said. Then, after string theorists found an answer, the mathematicians proved it on their own terms."
Many years ago I came across a simple version of this: If P is a convex polyhedron, with a distribution of mass and a center of mass C, then there exists a face F such that the line passing through C perpendicular to the plane of F lands in F.
The physics justification is that P can't roll for ever, so where ever it rests must be such an F. Even as a mathematician I was convinced, others were not.
The math proof is messier.
 
  • #64
Zafa Pi said:
You've held that position for quite a while now. Perhaps it's time for a change.:rolleyes:Those positions are far from universally accepted (e.g., Planck length limitation), and sufficiently untestable to be "not even wrong".

With a slightly amended set theory beyond ZFC all of analysis can be done with infinitesimals and thus countable. If you were raised with that orientation, then continuous would mean something different.
The usual real numbers are merely "a thinking tool", and should be kept from reality with likes of the tooth fairy.:smile:
Have you seen this? https://arxiv.org/abs/1609.01421

Speaking of set theory beyond ZFC, perhaps you could also add something here: https://www.physicsforums.com/threads/is-there-a-decidable-set-theory.939216/
 
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  • #66
Demystifier said:
objective reality may be continuous, but it just can't be measured.
Objective reality might also be discrete, but it just can't be decided by measurement. See my answer at https://physics.stackexchange.com/a/35676/7924

But almost all of physics assumes continuity, for very good reasons: The discrete case is essentially untractable since analysis (the tool created by Newton, in a sense the father of modern physics) can no longer be applied.
 
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  • #67
Zafa Pi said:
With a slightly amended set theory beyond ZFC all of analysis can be done with infinitesimals and thus countable. If you were raised with that orientation, then continuous would mean something different.

Nonstandard analysis is another way of proving the same theorems as ordinary analysis. The elements are not really "countable" in the sense that you can count them using finite numbers---you have to go to hyperfinite numbers.

It is nice that nonstandard analysis allows us to prove things using more intuitive (to many people) reasoning about infinitesimals, rather than limits, but it's really equivalent.
 
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  • #68
Zafa Pi said:
Ballentine makes it clear that physics consists of both a mathematical model and a correspondence to the physical world.
Claiming "physics is a mathematical model" is likely to hurt the feelings of experimentalists.
As a theorist, without hurting myself or my colleagues, claim the opposite: Physics is an empirical science in the fortunate position to have an astonishingly far-reaching theoretical description of the empirical findings ;-))).
 
  • #69
@Demystifier Just one more thing. Am I correct that if we consider the measurement on a pure state ##\rho = | \psi \rangle \langle \psi |## which results in $$\rho \rightarrow \tilde{\rho} := \frac{\int_{\mathcal{M}}A_C \rho A_C^{\dagger}dC}{Tr[\int_{\mathcal{M}}A_C \rho A_{C}^{\dagger}dC]}$$ Then if ##\tilde{\rho}## is a pure state as well then we can consider the change of the state ##| \psi \rangle## after measurement to be $$|\psi \rangle \rightarrow |\tilde{\psi} \rangle = \frac{1}{\mathcal{N}} \int_{\mathcal{M}} A_C | \psi \rangle dC?$$ where ##\tilde{\rho} = | \tilde{\psi} \rangle \langle \tilde{\psi} |##.
 
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  • #71
Well, the final statement in #70 is the socalled "collapse postulate". One should be aware that the validity of this assumption at best holds in a simplified sense for very special kinds of measurements, named von Neumann filter measurements, named after John von Neumann, who wrote a partially brillant book on the mathematical foundations of QT, establishing the Hilbert-space formalism, clarifying the somewhat delicate issue of unbound operators with continuous spectra. The physical part of this book, however, is partially misleading, precisely because of the issues with the collapse, quantum-classical cut, of some naive flavors of the Copenhagen interpretation.
 
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  • #72
A. Neumaier said:
Objective reality might also be discrete, but it just can't be decided by measurement. See my answer at https://physics.stackexchange.com/a/35676/7924
Agreed.
A. Neumaier said:
But almost all of physics assumes continuity, for very good reasons: The discrete case is essentially untractable since analysis (the tool created by Newton, in a sense the father of modern physics) can no longer be applied.
I would modify this with: "But almost all theories of physics ...
Physics in the lab is essentially discrete.
I've also read there is a program that simulates all of Newtonian mechanics (I'm still looking for it). Functions like cos and equations are subroutines. To get a definite answer the programs must halt giving discrete solutions. The real numbers never show up.

This article is interesting: https://www.wired.com/2009/04/Newtonai/
 
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  • #73
Hm, the stuff around me doesn't look very discrete to me. Also quantum theory, describing "discrete particles/quanta" is a theory described by continuum theories, i.e., (functional) calculus. What "nature really is" or what "objective reality" is, nobody can seriously say, and it's the realm of philosophical speculation rather than fact-based empirical natural science.
 
  • #74
vanhees71 said:
Hm, the stuff around me doesn't look very discrete to me.
I have never "seen" something non-discrete in my entire life. Even a "continuous" blue sky have to be distinguish from a "continuous" blue sheet of paper by its discrete borders...

vanhees71 said:
Also quantum theory, describing "discrete particles/quanta" is a theory described by continuum theories, i.e., (functional) calculus.
Indeed, but the question is that maybe a another type of math would better suit the problem of describing quanta of Nature.

vanhees71 said:
What "nature really is" or what "objective reality" is, nobody can seriously say
But do you agree that the goal of science is to deepen this knowledge ?. The stuff around me doesn't look very (im)probable to me. Yet I don't mind decreasing the scale of certain experiments until "probability" (or something like it) starts showing up.

vanhees71 said:
and it's the realm of philosophical speculation rather than fact-based empirical natural science.
Isn't it an undisputed fact that all observable are discrete ? Isn't it another fact that space/time coordinate and probabilities are abstraction (not facts) ?

For example a photon falling into a gravitational field will exchange its energy with the "continuous" field in a discrete manner. Isn't it actually falling down some stairs more than some space ?

For the records when I begin my computer career I was a full believer in continuum, and was wondering if the "abstract information/bits" mentality wasn't polluting all kind of sciences. I have completely changed my mind. A fact I learned soon enough is that some abstract continuous thing like a "real" won't fit any set of (f)actual bits (whatever the number of them 8-16-32...)

The Planck constant is staring us in the face for more then a century, and the Universe "facts" are made of light and matter ... not field nor probability.
 
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  • #75
vanhees71 said:
Hm, the stuff around me doesn't look very discrete to me.
You need to get refitted with glasses giving you 20/1035 vision.
 
  • #76
Zafa Pi said:
You need to get refitted with glasses giving you 20/1035 vision.
Did you mean... 6.096/3.04835 vision ?
 
  • #77
OCR said:
Did you mean... 6.096/3.04835 vision ?
Those would only cost half as much
 
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  • #78
Zafa Pi said:
Those would only cost half as much
No... !
They would cost two as much...

Zafa Pi said:
giving you 20/1035
OCR said:
Did you mean... 6.096/3.04835... ?
I think you are being contentious, and trying to make me look as a spectacle, simply because your unit is so short...

Zafa Pi said:
You need to get refitted with glasses giving you 20/1035 vision.
Lol, I'll bet if I wore those glasses, and stood on your shoulders... I could really see alot ... . :-p

.
 

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