Why does Quantum Mechanics have objective statistical characteristic?

In summary, Quantum Mechanics has two axioms that involve linear operators and state operators. These axioms lead to Gleason's Theorem, which shows that deterministic theories are not possible in QM. Non-contextuality is a crucial assumption in understanding the probabilities in QM, and without it, hidden variables or sub-quantum processes would be necessary to explain the results of measurements. Therefore, QM does not make a definitive statement on whether the microworld is deterministic or undeterministic, but it does require non-contextuality to be valid.
  • #1
ndung200790
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Why does Quantum Mechanics have objective statistical characteristic,but does not have subjective statistical characteristic?

QM has two axioms:
1-To each dynamical variable there coresponds a linear operator,and the possible values of the dynamical variable are the eigenvalues of the operator.
2-To each state there coresponds a unique state operator.The average value of a dynamical variable r,represented by the operator R,in the virtual ensemble of events that may result from a preparation procedure for the state,represented by the operator rho,is:
<average R>=Tr(rho.R).

Can we deduce the objective statistical characteristic from these axioms?If it is so that,what does lead us to the second axiom?
 
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  • #2
The second axion follows from the first via Gleasons Theroem:
http://en.wikipedia.org/wiki/Gleason's_theorem

I don't know what you mean by objective and subjective characteristic. Determinism can be viewed as a special case of a probabilistic theory - it only allows 0 and 1 as the probabilities. Although it not usually presented that way the Kochen Specker theorem follows fairly readily from Gleasons theroem:
http://en.wikipedia.org/wiki/Kochen–Specker_theorem

It shows you can't have only 0 and 1 as your probabilities so deterministic theories are kaput - with out. There is actually one other thing that goes into Gleason - non contextuality - so it not quite true to say it follows from the first axiom. However since non-contextuality relies on being able define the expectation values of operators that depends only on the eigenvectors and not on what other eigenvectors are part of it it makes the first axiom mathematically a bit weird if its not true.

Thanks
Bill
 
  • #3
Despite of KS theorem,but I have heard that strictly speaking quantum mechanics keeps silent about whether microworld is deterministic or undeterministic.The probability is not only equal 0 and 1,but we can't say about deterministic or undeterministic characteristic of the world.Is that correct?
 
  • #4
ndung200790 said:
Despite of KS theorem,but I have heard that strictly speaking quantum mechanics keeps silent about whether microworld is deterministic or undeterministic.The probability is not only equal 0 and 1,but we can't say about deterministic or undeterministic characteristic of the world.Is that correct?

The KS theorem is really a corollary of Gleason's Theorem - although for some reason it's usually presented separate from it (possibly because its proof has a mystique of difficulty - but it's not too bad - a proof has been found that is not that demanding mathematically and can be followed by someone with the equivalent of first year university calculus - see for example - Hugh's - The Structure and Interpretation of Quantum Mechanics).

Anyway its validity rests upon an assumption called non contextuality. Its a very natural assumption within the mathematical Hilbert Space framework of QM. In fact if its not true you would probably say why use Hilbert spaces in the first place - non contexuality is rather weird if you want that mathematical framework. The thing is though physically its not that weird - in fact looked at that way it's rather reasonable.

Bottom line is hidden variable interpretations like Bohmian Mechanics exist that are contextual so its certainly possible for this to happen - but only if you assume something beyond the normal formalism ie hidden variables or something sub-quantum.

So the situation is this - if you do not assume some kind of hidden variable theory then KS implies you cannot say it has that value prior to observation because only hidden variables allow non contextuality. If you do then yea - you can assume it. That's what I mean by some sub-quantum process.

Added Later:

I just realized I didn't make clear why this non contextuality is such a big deal - I merely said it was. If you choose a Hilbert space as your framework then you expect the elements to tell us something about the results of measurement - technically this is defining a measure on the states. This should not depend on the particular basis the state happens to be expanded in terms of - this is an arbitrary man made thing and the physics should not depend on it. This assumption is called non contextuality. All by itself, via Gleason's Theorem, it implies Born's rule and Born's rule means you can't define just 0 or 1 on all states.

Thanks
Bill
 
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1. Why is probability a fundamental aspect of quantum mechanics?

Quantum mechanics is a theory that describes the behavior of particles at a microscopic level. Unlike classical mechanics, which deals with macroscopic objects, quantum mechanics introduces the concept of probability to explain the behavior of particles. This is because at the quantum level, particles do not have precise positions or velocities, and their behavior is described by a wave function that gives the probability of finding the particle in a certain state. Therefore, probability is a fundamental aspect of quantum mechanics.

2. How does the probabilistic nature of quantum mechanics relate to the principle of uncertainty?

The principle of uncertainty, also known as Heisenberg's uncertainty principle, states that it is impossible to know both the position and momentum of a particle with absolute certainty. This is due to the probabilistic nature of quantum mechanics, where the more precisely we know one property of a particle, the less we know about the other. Therefore, the uncertainty principle is a direct consequence of the probabilistic nature of quantum mechanics.

3. Can the probabilistic nature of quantum mechanics be explained by hidden variables?

Some scientists have proposed the idea of hidden variables, which are unknown properties that determine the behavior of particles in quantum mechanics. However, this idea has been experimentally disproven, and it has been shown that the probabilistic nature of quantum mechanics cannot be explained by hidden variables. The theory of quantum mechanics is based on the idea that particles behave probabilistically, and this has been confirmed by numerous experiments.

4. How do we know that the probabilistic predictions of quantum mechanics are accurate?

Quantum mechanics has been extensively tested and has consistently made accurate predictions about the behavior of particles. This has been confirmed by experiments such as the double-slit experiment and the Stern-Gerlach experiment. Additionally, the predictions of quantum mechanics have been used to develop technologies such as transistors and lasers, which have been proven to work accurately. Therefore, the probabilistic predictions of quantum mechanics are well-established and have been experimentally validated.

5. Can the probabilistic nature of quantum mechanics be explained by our lack of knowledge about the system?

No, the probabilistic nature of quantum mechanics cannot be explained by our lack of knowledge about the system. This is because quantum mechanics is a complete and self-consistent theory that accurately describes the behavior of particles. It is not just a result of our limited understanding, but rather a fundamental aspect of the universe. Additionally, the probabilistic predictions of quantum mechanics have been confirmed by experiments, which rules out the possibility of our lack of knowledge being the cause of the probabilistic nature of quantum mechanics.

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