Is the wavefunction subjective? How?

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In summary: But it is not 50% because you can't flip a coin twice and have it come out the same. So it is not 50% because it is not a real number. It is purely a representation of something that can only be determined by observation.This is similar to the wavefunction. There is a corresponding measurement that is guaranteed to give a particular result, if that's the correct wave function. If it gives anything else, that wave function was objectively wrong.
  • #36
stevendaryl said:
Yes, in Bayesian probability, you can be proved objectively wrong if you give an assignment of 0 or 1 to some possibility. So in that sense, Bayesian probability has an objective element to it, which is what is possible and what is not. The exact numbers are subjective.
I think the analogy is fairly direct as the pure states of classical probability theory, the point masses, have exactly the property you mentioned, i.e. always having some observable that can determine if they are wrong. Even a large class of mixed states, i.e. mixed states whose support is not the entire sample space, have this property
 
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  • #37
DarMM said:
I think the analogy is fairly direct as the pure states of classical probability theory, the point masses, have exactly the property you mentioned, i.e. always having some observable that can determine if they are wrong. Even a large class of mixed states, i.e. mixed states whose support is not the entire sample space, have this property

That's the reason I would say that quantum amplitudes are actually objective. They can always be proved wrong by a single measurement. (In contrast, other than 0 or 1 probabilities, no single observation can prove a Bayesian probability assignment wrong.)
 
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  • #38
bhobba said:
It shows it exits (providing non-contextuality is assumed) but says nothing about if its just subjective or real.
Do you think non-contextuality can be justified via no-signalling? If we made probability assignments that revealed the context and verified them we could know the settings of distant experiments.
 
  • #39
stevendaryl said:
That's the reason I would say that quantum amplitudes are actually objective. They can always be proved wrong by a single measurement. (In contrast, other than 0 or 1 probabilities, no single observation can prove a Bayesian probability assignment wrong.)
In Bayesian probability all pure states and a large class of mixed states (those with support on a strict subset) can be proven wrong with a single observation.
 
  • #40
DarMM said:
In Bayesian probability all pure states and a large class of mixed states (those with support on a strict subset) can be proven wrong with a single observation.

Isn't that what I said? (Except I said it in the language of probability 0 and probability 1)
 
  • #41
stevendaryl said:
Isn't that what I said? (Except I said it in the language of probability 0 and probability 1)
It's this part:
In contrast, other than 0 or 1 probabilities, no single observation can prove a Bayesian probability assignment wrong
I don't see how that is different from the quantum case or why it is a contrast.
 
  • #42
DarMM said:
I don't see how that is different from the quantum case or why it is a contrast.

Every quantum case corresponds to the perfect knowledge case of Bayesian probability, and the perfect knowledge case of Bayesian probability is objective.
 
  • #43
I get that, are you saying there is a difference in the quantum case or not?

All I mean is that there doesn't seem to be anything additional that quantum mechanics adds to the subjective/objective probability debate.
 
  • #44
DarMM said:
I get that, are you saying there is a difference in the quantum case or not?

All I mean is that there doesn't seem to be anything additional that quantum mechanics adds to the subjective/objective probability debate.

I really don't understand what's the difficulty. Bayesian probability becomes objective in the case where all probabilities are either 0 or 1. Quantum mechanics corresponds to this case. So it's objective.
 
  • #45
stevendaryl said:
I really don't understand what's the difficulty. Bayesian probability becomes objective in the case where all probabilities are either 0 or 1. Quantum mechanics corresponds to this case. So it's objective.
There's no difficulty. I'm saying that I don't think QM adds anything to the subjective/objective probability debate, i.e. it doesn't have anything new to say about that issue compared to classical probability theory.
 
  • #46
DarMM said:
There's no difficulty. I'm saying that I don't think QM adds anything to the subjective/objective probability debate, i.e. it doesn't have anything new to say about that issue compared to classical probability theory.

And I'm saying that you're wrong. If in classical probability, you only allowed 0 or 1 values for the probability, then probability wouldn't be considered subjective, since disagreements could be objectively resolved. Quantum mechanics is in this situation: Disagreements about the value of the wave function can be objectively resolved.
 
  • #47
stevendaryl said:
And I'm saying that you're wrong.
QM does add something to the debate then. What is it?
 
  • #48
stevendaryl said:
And I'm saying that you're wrong. If in classical probability, you only allowed 0 or 1 values for the probability, then probability wouldn't be considered subjective
That's not classical probability theory though, that's Boolean logic.

stevendaryl said:
Quantum mechanics is in this situation: Disagreements about the value of the wave function can be objectively resolved.
I don't get it, what is the feature QM has, mathematically, that classical probability lacks that adds something to the subjective/objective probability debate?
 
  • #49
DarMM said:
I don't get it, what is the feature QM has, mathematically, that classical probability lacks that adds something to the subjective/objective probability debate?

I really don't get what it is that you don't get. I've answered the question many times, and I guess to no avail. Quantum wavefunctions are objective, not subjective.
 
  • #50
stevendaryl said:
Um. I answered that question several times. I believe that the quantum wave function is objective. If I'm right, then doesn't that resolve the subjective/objective question?
Well obviously if the wave function is objective then it resolves the question.

I'm asking what features are you using that indicate quantum states are objective and classical probability states are not.

Let's look at equivalent states:
  1. Pure states. In both cases there are questions that definitively show you are correct or not
  2. Somewhat Mixed states. These are states with strict subset support in the classical case and states like ##\omega = \frac{1}{2}\left(\omega_1 + \omega_2\right)## (with ##d \geq 3## of course) in the quantum case. It can be possible to establish one's mixed state is wrong in a single observation.
  3. Highly mixed states. Probability measures with support on the whole sample space in the classical case, states like ##\mathbb{I}## in the quantum case. It is not possible to establish you are wrong in one measurement.
To me they seem the same.
 
  • #51
stevendaryl said:
In contrast, other than 0 or 1 probabilities, no single observation can prove a Bayesian probability assignment wrong
Basically I think you are comparing quantum pure states with high entropy classical states with some assignment to all outcomes and concluding objectivity. Rather you should compare like with like. All quantum states with all classical states. Then you will see there is no difference.

Bayesian probability assignments which cover the whole sample space are analogous to mixed states in quantum mechanics, thus there is no difference. You shouldn't compare these to pure states.
 
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  • #52
stevendaryl said:
And I'm saying that you're wrong. If in classical probability, you only allowed 0 or 1 values for the probability, then probability wouldn't be considered subjective, since disagreements could be objectively resolved. Quantum mechanics is in this situation: Disagreements about the value of the wave function can be objectively resolved.
This might be the post to focus on, disagreements about mixed quantum states can't be resolved in one measurement in general, just as classical probability distributions can't be discarded in one measurement in general.

However in both cases, quantum and classical, there is a subset of mixed states (of which pure states are a special case) which can.

stevendaryl said:
Every quantum case corresponds to the perfect knowledge case of Bayesian probability, and the perfect knowledge case of Bayesian probability is objective.
Basically they don't. Quantum pure states correspond to the perfect knowledge case, quantum states in general do not.
 
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  • #53
DarMM said:
Do you think non-contextuality can be justified via no-signalling? If we made probability assignments that revealed the context and verified them we could know the settings of distant experiments.

I think Kochen-Specker basically says that - but a deeper analysis than I am aware of may show there is an out to that one. Personally I find contextuality ugly which is one reason I do not like interpretations that have it. The way these threads often go forces me to emphasize my dislike for something means absolutely nothing - its simply an opinion. Nature could indeed be contextual.

Thanks
Bill
 
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  • #54
stevendaryl said:
And I'm saying that you're wrong. If in classical probability, you only allowed 0 or 1 values for the probability, then probability wouldn't be considered subjective, since disagreements could be objectively resolved. Quantum mechanics is in this situation: Disagreements about the value of the wave function can be objectively resolved.

Only by people who agree on the same objective facts.
 
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  • #55
atyy said:
Only by people who agree on the same objective facts.
And for them to reach such an agreement they must coexist in the same classical background; where the "quantum inquiries" are defined. And there interactions for all practical purposes be classical.

This is clearly a scenario that does not cover general cases of inside observers, so this stance will not be viable in the QG or unification realm I would say.

/Fredrik
 
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  • #56
atyy said:
Only by people who agree on the same objective facts.
Fra said:
And for them to reach such an agreement they must coexist in the same classical background; where the "quantum inquiries" are defined. And there interactions for all practical purposes be classical.

This is clearly a scenario that does not cover general cases of inside observers, so this stance will not be viable in the QG or unification realm I would say.

/Fredrik
People agreeing on objective facts is basic requirement for doing science. You can not relax this stance and still pretend that your philosophy has something to do with science.
 
  • #57
zonde said:
People agreeing on objective facts is basic requirement for doing science. You can not relax this stance and still pretend that your philosophy has something to do with science.
I think what they mean is given a cut, or what Healey calls "the physical situation of the agent", there is a best wavefunction.

In other words given what you currently know there is a "best" wavefunction you should be using like Objective Bayesianism. However agents in two different physical situations (i.e. one will have witnessed a different set of events) won't have the exact same quantum state. Just like Classical Probability Theory.
 
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  • #58
zonde said:
People agreeing on objective facts is basic requirement for doing science. You can not relax this stance and still pretend that your philosophy has something to do with science.
If we are literally speaking of "people" or scientists, they all coexist on the same classical background, and can fapp communicate and compare their observations classically - this is of course not where the problem lies.

"People" here is a metaphor for a information processing agent - a generalisation of an observer - but one that is not necessarily "classical".

Quantum mechanics as it stands relies on a classical background and classical measurement device to be defined. This was i think understood by many of the founders of QM, but often misinterpreted to somehow involve humans or "minds".

We do not need to make the same mistake again. The above paradigm is IMO not making sense in QG, unification attempts or cosmological models. So we desperately NEED to reconstruct a measurement theory, in terms of a non-classical observer. Observers that moreoever is interacting with other observers. The correspondence is that we must recover regular QM and QFT in the appropriate limit of a dominant classical lab frame observer observing a small subsystem.

But we still lack the framework to describe this. But one trait of such a framework is indeed that effective truth values are not necessarily objective. But we should not interpret this as the breakdown of effective human science, i think it rather deepens our understanding to see how "objectivity" can emergent, from a chaotic starting point. That BIG difference is that in this paradigm, the objectivity are NOT hard god given mathematical constraints that need no explanation.

/Fredrik
 
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  • #59
Fra said:
But we should not interpret this as the breakdown of effective human science, i think it rather deepens our understanding to see how "objectivity" can emergent, from a chaotic starting point.
Absence of "objectivity" is subjectivity not chaos. But for any "objectivity" to emerge we need fapp objective communication channels to compare our subjective observations. So we have to assume at least some objectivity to start talking about emergence of "objectivity". This makes your idea about emergent "objectivity" circular.
 
  • #60
zonde said:
Absence of "objectivity" is subjectivity not chaos. But for any "objectivity" to emerge we need fapp objective communication channels to compare our subjective observations. So we have to assume at least some objectivity to start talking about emergence of "objectivity". This makes your idea about emergent "objectivity" circular.

Yes the subjectivity is the unavoidable observer choice but this is really something you can not escape unless you engage in ontological fantasy. I require that ontologies are the result of a physical inference process, otherwise it is to me metaphysics.

Any comparasiom between two subjective views takes a third perspective. And comparasions are necessarily physical interactions.

This is a chicken and egg situation but circular is i think a bad an inappropriate descriptor as it sounds like a deadlock which it ia not.

I call i evolving. Evolving means progress and revision is made on each comparasion rather than contradictions. Agents that don't revise and negotiate will not be stable and thus not be abundant in nature.

/Fredrik
 
  • #61
Fra said:
This is a chicken and egg situation but circular is i think a bad an inappropriate descriptor as it sounds like a deadlock which it ia not.
Let's not say that "it does not work" because it sounds like it does not work while I think that it works? - is this what you are saying?

Do you have some valid starting point for your reasoning? What is instead of what is not? And is it consistent with scientific approach? It does not seem so to me.

You have to understand that science does not cover all the thinkable explanations of the world. It covers only limited class of explanations. And it does not seem that your reasoning is anywhere near that "limited class of explanations".
 
  • #62
zonde said:
People agreeing on objective facts is basic requirement for doing science. You can not relax this stance and still pretend that your philosophy has something to do with science.

"People" is subjective. What is a person?
 
  • #63
atyy said:
"People" is subjective.
In what sense "people" is subjective?
atyy said:
What is a person?
For example me and you. A person who does the science is a primitive term in context of philosophy of science so it does not require definition.
 
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  • #64
Basically I think one can argue that given a particular cut/physical situation/observed outcomes that there is a best wavefunction. The same kind of thing Jeffreys and Jaynes had for Classical Probability.

However because there is a Quantum de Finetti theorem you are also fine taking it subjectively like Savage, Ramsey and de Finetti did for Classical Probability.

So you just fall back to the interpretation of Probability theory in general.
 
  • #65
DarMM said:
Basically I think one can argue that given a particular cut/physical situation/observed outcomes that there is a best wavefunction.
This is not sufficient: Taking the cut to include a lot (system, detector, much environment), the corresponding best wave function should determine all probabilities about (system, detector, much environment), and hence should determine all conditional probabilities when taking the cut more narrowly, e.g., only (system, detector). But this conditional probability is not given by a wave function.
 
  • #66
A. Neumaier said:
This is not sufficient: Taking the cut to include a lot (system, detector, much environment), the corresponding best wave function should determine all probabilities about (system, detector, much environment), and hence should determine all conditional probabilities when taking the cut more narrowly, e.g., only (system, detector). But this conditional probability is not given by a wave function.
Could you describe what you mean in a bit more detail?
 
  • #67
"The wave function cannot be measured (its tiny changes cannot be distinguished by any apparatus that studies the physical system once) which is a good reason to say that "it probably doesn't objectively exist"

Basically, In this sense the complex conjugate square of the wave function that gives the probability for an event to happen, is objective. It is a real number and accumulating measurements with the same conditions always gives the same probability distribution, even though there are levels upon levels of modeling. The wavefunction is the mathematical modeling of what happens when "particle scatters" . It is not the wavefunction that interacts, it is the particle(blurry bunch) which interacts with the boundary conditions of a experiment that can be fitted with a wavefunction which complex conjugate squared gives the probability distribution for the experiment.
 
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  • #68
zonde said:
In what sense "people" is subjective?

For example me and you. A person who does the science is a primitive term in context of philosophy of science so it does not require definition.

"People" is subjective like "measurement apparatus".
 
  • #69
zonde said:
Let's not say that "it does not work" because it sounds like it does not work while I think that it works? - is this what you are saying?
No, I was basically saying that I read your understanding of "objectivity" as what from my perspective is a deceptive illusion.

But I was trying to put it in more polite manner for the sake of discussion by saying that you make and observation that I partially agree with (that we have a self-referencing situation), but when you say its circular that implies to me you are missing the point.
zonde said:
Do you have some valid starting point for your reasoning? What is instead of what is not? And is it consistent with scientific approach? It does not seem so to me.

You have to understand that science does not cover all the thinkable explanations of the world. It covers only limited class of explanations. And it does not seem that your reasoning is anywhere near that "limited class of explanations".
To connect this to the scientific method, what I am talking about here belongs to the hypothesis generation part. This is the part that Popper tried to sweep under the rug byt instead focus on the deductive falsification events.

But if you have given unification approaches and thoughts you should know that one problem is that faces initial value problems, problems with naturalness etc, simple BECAUSE the state spaces are so large. As smolin etried to explain to death in books, this is a failure of what he calls the Newtonian paradigm. It is actually also related to the "unreasonable effectiveness of mathematics", which when you understand the reason for it is in fact very reasonable. Its effective because it applies to subsystems.

As I said, no one has yet published a theory of framework for this, that to my knowledge is a solution. But let's not avoid facing the problem just because we have no solution.

My staring point means to reconstruct a measure framework, from the perspective of a ficitve information processing agent. This has the advantage that as you scale down the complexity, the state space is NOT infiinte, it rather gets trivially small. The challenge is then to see how relation emerge as these interact and gain complexity. This process of scaling complexity corresponds exactly to the big band and TOE unification level: information processing agents are like spieces that POPULATE the universe, and they are further assocaite to elementary particles, and their RELATIONS encode also spacetime. The Science here is that this is a hypothesis, if this works and reproduces known physics or reducing the number of free parameter,, and thus increases the explanatory power, then it will also yield more predictions that can be tested.

But you can not apply Poppian falsification logic to the process of hypothesis generation! This is not how creative or evoltionary processes work. Most scientis keeps these dirty thoughts to themselves, and only present the "result".

/Fredrik
 
  • #70
stevendaryl said:
Saying that probabilities are relative frequencies doesn't really make sense.

And defining a probability as the relative frequency of an event in a specific population doesn't produce a model of the probability of that event occurring in a "random" trial unless we assume there is a mechanism for independently selecting a member of that population that gives each member of the population the same probability of being selected. So the frequency definition of probability requires a non-frequency concept of probability in order to handle the usual applications of probability.
 
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