High School Meaning of Wave Function Collapse

Click For Summary
Wave function collapse refers to the process by which a quantum system's state becomes definite upon measurement, often leading to confusion due to its terminology. The term "collapse" can mislead laypeople into thinking of a physical process, whereas it simply indicates that a measurement has occurred, resulting in a specific value. This confusion is compounded by other loaded terms like "observation" and "particle," which have historical roots that may not align with modern understanding. The discussion emphasizes the need for grounding quantum mechanics in comprehensible terms while acknowledging that some concepts may inherently resist non-mathematical explanations. Ultimately, the complexity of wave function collapse reflects broader mysteries in physics that may never be fully resolved.
  • #31
PeterDonis said:
Those don't say "collapse" in the sense @bhobba was using the term is part of QM. They say that the von Neumann projection postulate is part of QM. That's not the same thing. The projection postulate makes no claims about whether "collapse really happens"; it just says that, in the mathematical formalism, once you observe a particular measurement result you have to use the projection postulate to get the system's new quantum state that you will use to predict the probabilities of future measurement results.

In both posts #18 and #26, @bhobba does not mention collapse as being real.
 
Physics news on Phys.org
  • #32
ZapperZ said:
The problem with QM has always been with people who do not know QM (i.e. the mathematical formalism)

The question of whether particles possesses specific states in between interactions/observations/measurements is not a problem with QM. Its just a question. Wanting an answer to that question, in my view, is not a critique of QM mathematical formalism. If you are saying an understanding of the math will render that question irrelevant to the individual who understands the math, I don't see that path, myself. I have only a coarse understanding of the math, admittedly.
 
  • Like
Likes Boing3000
  • #33
atyy said:
In both posts #18 and #26, @bhobba does not mention collapse as being real.

He said in #18 that "collapse" as he was using it is not part of basic QM, only of some interpretations. That means he wasn't using it, at least not in that post, to refer to the projection postulate, which is part of basic QM.

He also said in post #26 that he was willing to use your definition of the term "collapse" in the future, if you post it here. My own preference would be to reserve the term "collapse" for the thing that "collapse interpretations" use that term to mean (i.e., not the projection postulate, but some stronger claim that would more or less amount to saying that some form of collapse "really happens"), and to use some term like "projection postulate" for the "collapse" that's part of basic QM. But I think the main thing is that everyone agrees on some consistent use of terminology, whatever that is.
 
  • Like
Likes rubi and bhobba
  • #34
I would disagree with Zapperz that the formalism came first, and also "It is the interpretation that is trying to put into words what the formalism presents!" QM effectively started with Planck, Einstein, Bohr/Sommerfeld (on a wrong track), de Broglie then Schrödinger, and we generally agree that the Schrödinger equation, in the form Schrödinger presented it, and the Uncertainty Principle (which in my opinion is actually implied by the Schrödinger equation) came first and essentially contains quantum mechanics. The formalism followed. Interpretation might involve what the formalism means in some eyes, but to me interpretation falls back to what does ψ mean? In my opinion, there are three basic interpretations, with a variety of variations to each. First there is the fundamental question, is there actually a wave or is it merely a mathematical artefact? De Broglie/Bohm, (and for that matter, me) consider that there is a wave (but that raises problems because where is it and why can't we detect it?) while most seem to say, no, there isn't, but that raises problems as to what actually causes diffraction? The probabilistic view works well mathematically, but it does not explain how the probabilities arise, or, for that matter, how they resolve. All of these issues are independent of formalism, but of course if you have used said formalism consistently, you probably feel very comfortable with it.
 
  • Like
Likes richrf
  • #35
Grinkle said:
The question of whether particles possesses specific states in between interactions/observations/measurements is not a problem with QM. Its just a question. Wanting an answer to that question, in my view, is not a critique of QM mathematical formalism. If you are saying an understanding of the math will render that question irrelevant to the individual who understands the math, I don't see that path, myself. I have only a coarse understanding of the math, admittedly.

Now it appears that the issue that you have brought up is going in a different direction. You are now talking not about "collapse", but rather superposition. Do you really want to do this?

I didn't say anything about individuals who understand the QM formalism and consequently do not have question about what is going on, even though many in the "Shut Up And Calculate" camp would be waving their hands. But from my experience on here for all the many years, a lot of the question on "collapse", on "schrodinger cat", on "entanglement", etc... etc. were major concerns with people who do not understand the QM formalism FIRST before moving on in trying to figure out that that formalism means. It is like you're having a problem with a story that you've only heard told via 3rd hand news, in a different language than what it was originally. You can't construct a solid understanding when the starting point is simply a superficial idea of it. But yet, these are usually the people who demand that we give them a clear and an unambiguous answer to their questions.

Zz.
 
  • Like
Likes bhobba
  • #36
Ian J Miller said:
I would disagree with Zapperz that the formalism came first, and also "It is the interpretation that is trying to put into words what the formalism presents!" QM effectively started with Planck, Einstein, Bohr/Sommerfeld (on a wrong track), de Broglie then Schrödinger, and we generally agree that the Schrödinger equation, in the form Schrödinger presented it, and the Uncertainty Principle (which in my opinion is actually implied by the Schrödinger equation) came first and essentially contains quantum mechanics. The formalism followed. Interpretation might involve what the formalism means in some eyes, but to me interpretation falls back to what does ψ mean? In my opinion, there are three basic interpretations, with a variety of variations to each. First there is the fundamental question, is there actually a wave or is it merely a mathematical artefact? De Broglie/Bohm, (and for that matter, me) consider that there is a wave (but that raises problems because where is it and why can't we detect it?) while most seem to say, no, there isn't, but that raises problems as to what actually causes diffraction? The probabilistic view works well mathematically, but it does not explain how the probabilities arise, or, for that matter, how they resolve. All of these issues are independent of formalism, but of course if you have used said formalism consistently, you probably feel very comfortable with it.

Sorry, you have a misunderstanding of what "formalism" means, at least in the way that I've used it. Formalism is the mathematical description. So the Schrodinger equation is part of the QM formalism. The mathematics of QM came first. Then people tried to figure out what those means.

Zz.
 
  • #37
ZapperZ said:
Now it appears that the issue that you have brought up is going in a different direction.

You have me confused with someone else, I think. As far as I know, I didn't bring up any issues in this thread.
 
  • #38
Grinkle said:
You have me confused with someone else, I think. As far as I know, I didn't bring up any issues in this thread.

You said:

The question of whether particles possesses specific states in between interactions/observations/measurements is not a problem with QM.

That's quantum superposition, is it not? That's not what is being asked in this thread, i.e. "collapse" of the wavefunction upon measurement.

Zz.
 
  • #39
ZapperZ said:
That's quantum superposition, is it not? That's not what is being asked in this thread, i.e. "collapse" of the wavefunction upon measurement.

I see. So you can understand my "B" level thinking - When I hear "collapse" I picture the possibility that pre-collapse there was no well defined state of the particle and post-collapse there is.

So the question that occurs to me is whether that pre/post collapse transition is 'real' or whether there was a well defined state all along. I didn't realize I was talking about a different thing altogether than collapse.

In any case, my point was not that I am owed an answer from QM. My point is that asking such a question is not the act of saying there is a problem with QM.

I can accept that my questions are poorly posed. Instead of wasting folks time honing my layman's phrasing, I will watch with interest any discussion on the below question.

Ian J Miller said:
is there actually a wave or is it merely a mathematical artefact?
 
  • #40
Grinkle said:
I see. So you can understand my "B" level thinking - When I hear "collapse" I picture the possibility that pre-collapse there was no well defined state of the particle and post-collapse there is.

So the question that occurs to me is whether that pre/post collapse transition is 'real' or whether there was a well defined state all along. I didn't realize I was talking about a different thing altogether than collapse.

In any case, my point was not that I am owed an answer from QM. My point is that asking such a question is not the act of saying there is a problem with QM.

I can accept that my questions are poorly posed. Instead of wasting folks time honing my layman's phrasing, I will watch with interest any discussion on the below question.

But if you want "answers" on superposition or whether it is "real" (it is), then you should scour the numerous threads we already have on that topic or the topic of Schrodinger cat, which is basically an attempt at illustrating the issue of quantum superposition. Do a search on Delft/Stony Brook experiments on SQUIDs and the measurement of the coherence gap, which would not be there if quantum superposition doesn't occur.

But this is not what the OP asked in this thread.

Zz.
 
  • Like
Likes bhobba
  • #41
ZapperZ said:
But if you want "answers" on superposition or whether it is "real"

Yes, I am confident I can find a lot of good material with a thread search. It was not my intent to change the topic of this thread.
 
  • #42
PeterDonis said:
But I think the main thing is that everyone agrees on some consistent use of terminology, whatever that is.

Right, that's all that's needed. We do not want to confuse anyone, just discuss and/or help people with physics. I am happy with any reasonable view, just as long as we all stick to it.

Thanks
Bill
 
  • #43
bhobba said:
Right, that's all that's needed. We do not want to confuse anyone, just discuss and/or help people with physics. I am happy with any reasonable view, just as long as we all stick to it.

Thanks
Bill

So is the projection postulate common to all interpretations?
 
  • #44
atyy said:
So is the projection postulate common to all interpretations?

Under the following definition yes:

The postulate in quantum mechanics that observation of a physical system, by determining the value of an observable, results in the transition of the quantum state of the system to a particular eigenstate corresponding to the eigenvalue of the observed quantity.

But IMHO its not a postulate - it comes from the two axioms of Ballentine.

Thanks
Bill
 
  • #45
bhobba said:
Under the following definition yes:

The postulate in quantum mechanics that observation of a physical system, by determining the value of an observable, results in the transition of the quantum state of the system to a particular eigenstate corresponding to the eigenvalue of the observed quantity.

But IMHO its not a postulate - it comes from the two axioms of Ballentine.

Thanks
Bill

What is the difference between "collapse" (in your language) and the projection postulate?
 
  • #46
atyy said:
What is the difference between "collapse" (in your language) and the projection postulate?

According to John Von-Neumann its basically the same thing.

Thanks
Bill
 
  • #47
bhobba said:
The postulate in quantum mechanics that observation of a physical system, by determining the value of an observable, results in the transition of the quantum state of the system to a particular eigenstate corresponding to the eigenvalue of the observed quantity.

Note carefully, though, that as far as basic QM (i.e., without any interpretations, just calculating predictions) is concerned, "transition of the quantum state" does not mean the actual system's state necessarily changes. It's only a transition in the mathematical model--the machinery you use to make predictions about future measurement results. Whether or not that transition in the model corresponds to a "real" transition in the system being modeled is interpretation dependent. Unfortunately, it takes a lot of care and precision in language to keep this distinction clear, since the usual ordinary language we use to talk about this stuff leaves it ambiguous.
 
  • Like
Likes Grinkle, rubi and bhobba
  • #48
PeterDonis said:
It's only a transition in the mathematical model--the machinery you use to make predictions about future measurement results. Whether or not that transition in the model corresponds to a "real" transition in the system being modeled is interpretation dependent.
It can't be interpretation dependent. Think of three polarizers experiment where you have two orthogonal polarizers and insert the third between. The change in observed result between two polarizers and three polarizers setups is real. Interpretation has to predict it. How would any current interpretation predict it without a physical transition in the system being modeled?
 
  • #49
zonde said:
How would any current interpretation predict it without a physical transition in the system being modeled?
A polarizer isn't modeled by a projection, but by unitary evolution. A projection is only required when we obtain information. Most physicists interpret it as an update of (quantum) information, rather than a physical process.
 
  • Like
Likes atyy and bhobba
  • #50
rubi said:
A polarizer isn't modeled by a projection, but by unitary evolution.
Let's treat the first polarizer as state preparation so that we have pure H polarized state after the first polarizer. After the second polarizer the state is say in superposition of being +45deg and absorbed by the second polarizer + being -45deg and passed through the second polarizer. Is it ok so far? Now how do you model interaction with the third polarizer. Only the part that passed the second polarizer interacts with the third polarizer. Or no?
 
  • #51
zonde said:
Let's treat the first polarizer as state preparation so that we have pure H polarized state after the first polarizer. After the second polarizer the state is say in superposition of being +45deg and absorbed by the second polarizer + being -45deg and passed through the second polarizer. Is it ok so far? Now how do you model interaction with the third polarizer. Only the part that passed the second polarizer interacts with the third polarizer. Or no?
Every polarizer ##i## has an associated unitary operator ##U_i##. You start with a state ##\psi##. After the first polarizer, the state it ##U_1\psi##. After the second one, it is ##U_2 U_1\psi## and after the third polarizer, it is ##U_3 U_2 U_1\psi##. No projections are involved. You have to insert projections only if you perform measurements in between.
 
  • Like
Likes dextercioby, bhobba and atyy
  • #52
rubi said:
Every polarizer ##i## has an associated unitary operator ##U_i##. You start with a state ##\psi##. After the first polarizer, the state it ##U_1\psi##. After the second one, it is ##U_2 U_1\psi## and after the third polarizer, it is ##U_3 U_2 U_1\psi##. No projections are involved. You have to insert projections only if you perform measurements in between.
And what are the components of the state ##U_3 U_2 U_1\psi##? One component has to have amplitude who's square is 1/8 given common polarizer angles for this example (H, 45deg, V)
 
  • #53
zonde said:
And what are the components of the state ##U_3 U_2 U_1\psi##? One component has to have amplitude who's square is 1/8 given common polarizer angles for this example (H, 45deg, V)
Well, I'm too lazy right now to write down all the matrices and perform the calculation, but of course, if you choose ##U_i## and ##\psi## correctly and then expand the final state in the basis of your choice, you will get the correct experimental predictions.
 
  • Like
Likes atyy
  • #54
bhobba said:
As defined in the standard textbook - Decoherence and the Quantum-to-Classical Transition by Maximilian A. Schopenhauer:

I think you surely meant “Schlosshauer” and not the German philosopher Arthur Schopenhauer (1788 – 1860) (https://en.wikipedia.org/wiki/Arthur_Schopenhauer). :wink:

Nevertheless, Schopenhauer’s reasoning and transcendental idealism might be of interest with respect to discussions about quantum mechanics. Schopenhauer described transcendental idealism as a "distinction between the phenomenon and the thing in itself", and a recognition that only the phenomenon is accessible to us because "we know neither ourselves nor things as they are in themselves, but merely as they appear.”
 
  • Like
Likes vortextor, dextercioby, bhobba and 2 others
  • #55
Peter Morgan said:
One way to ground everything in reality is to think purely about the records of experiments that are stored in computer memory. Very often, that's a list of times at which events happened. If you think about APDs, for such devices we might run a wire (or we use a fiber optic cable, or wi-fi, ...) from the APD to the computer that records the data. On that wire, there will be a voltage that most of the time will be near zero voltage, but occasionally an "avalanche" happens, the voltage goes to non-zero (1 volt, 20 volts, whatever), then the hardware checks a clock for the time and records it in memory and then to hard disk for later analysis. The hardware also resets the APD as soon as possible so another avalanche can happen. From a computing and signal analysis point of view, what's just happened was a compression: we could have recorded the voltage picosecond by picosecond to 14-bit accuracy, but we just recorded the time when there was a signal transition from zero to not-zero.
There are certainly experiments that record continuous signals (at finite accuracy and resolution, with a fixed schedule, because it's all going into digital memory), but the analyses that you'll find detailed in physics papers are often on the hunt for discrete structure of some kind, and very often a discrete structure is there to be found.

Everything so far is classical electronics (except the last sentence, which presaged what comes next here) about events and signals. There is no mention of particles or of particle properties whatsoever. Now comes the analysis, where we will introduce the idea that particles (or, more generally, "systems", a field, thing or things that are kinda classical) explain why we see the events and signals that we see. The Correspondence Principle gives us a way, called quantization, to convert a classical dynamics for some kind of classical system (mechanics or electromagnetism) into a differential equation that describes the evolution over time of a "statevector", the Schrödinger equation. The statevector models/predicts the statistics of many different kinds of measurement results (anything that can come out of a mathematical analysis of the raw data of the previous paragraph), and, crucially, how they change over time. Some of those measurement results are "incompatible" with each other, so that properly speaking we can't talk about correlations between incompatible measurements.
The Correspondence Principle is quite tricky because it cannot be a perfect map from a classical dynamics to a quantum dynamics, but it's been a fairly decent guide for the last 90 years, so we're not going to give it up until we have something better. If we find that the quantization of a classical mechanics works well as a model for the signal analysis we do for the raw data, which has to work nicely as the statistics change over time, we pretty much say that the quantized classical system explains the raw data, except of course that we don't as much understand what we're doing when we quantize as we'd like to.
So, @Carpe Physicum, it looks as if you might have left this conversation. If you're still here, I hope you find this a little useful even though it's definitely my idiosyncratic way of thinking about the question. I've tuned the above a little to the computing world because that seems to be your sort of thing, which wasn't hard to do, however, because that's also pretty close to my sort of thing. If you reply, I can point you to the first video on my YouTube channel. I'm trying to figure out whether you really mean Carpe, or perhaps there's a little Carping in your question?:wink:
Sorry I did drop for a bit. Very interesting and informative. As a layman it always is amazing how theory and brute reality, as in where the data actually comes from and how it's used, how those two relate. As for the name, yes Carpe, Seize The Physics! (in broken latin of course :) )
 
  • Like
Likes zonde
  • #56
rubi said:
Every polarizer ##i## has an associated unitary operator ##U_i##. You start with a state ##\psi##. After the first polarizer, the state it ##U_1\psi##. After the second one, it is ##U_2 U_1\psi## and after the third polarizer, it is ##U_3 U_2 U_1\psi##. No projections are involved. You have to insert projections only if you perform measurements in between.

Are you talking about a special kind of polarizer, or the usual "polarizing filter" (such as is used in some sunglasses)? In the usual kind of polarizing filter, light that is polarized one way passes through unchanged, while light that is polarized perpendicular to that is absorbed by the filter. Absorption of a photon is irreversible, which usually means it is not described by a unitary transformation. Maybe I'm misunderstanding what you're saying?

I think there are devices that simply rotate the polarization of incoming light, without absorption.
 
  • #57
I try to explain what "collapse of the wave function" means without entering "semantic" discussions.
Take a coin and throw it. While the coin is launched, it has no value, it is, so to speak, both head and cross. Since the head and the cross are 1/2 chance to exit, we can formalize the "state" of the coin as a linear combination of "heads" and "cross": indicating with ## \psi ## the wave function of the coin we can write:
## \psi = 1/2H+1/2C ##
where C means cross, H, head, and 1/2 is the probability factor that exits H (or C).
Suppose the coin lands on a table and you say, "Oh, head out!"
Then the wave function, which was ##\psi ## before became H.
In other words there has been a reduction (or collapse) from ## \psi ## to H
Or, mathematically formalizing:
##\psi \rightarrow H ##
This is the "collapse" of the wave function, neither more nor less
 
  • #58
stevendaryl said:
Are you talking about a special kind of polarizer, or the usual "polarizing filter" (such as is used in some sunglasses)? In the usual kind of polarizing filter, light that is polarized one way passes through unchanged, while light that is polarized perpendicular to that is absorbed by the filter. Absorption of a photon is irreversible, which usually means it is not described by a unitary transformation. Maybe I'm misunderstanding what you're saying?

I think there are devices that simply rotate the polarization of incoming light, without absorption.
Well, polarizers are understood quite well quantum mechanically in solid-state physics. What happens during an absorption is that photons are scattered into phonons, i.e. lattice vibrations, in the polarizer and the photon-phonon cross section is higher if the photon is polarized appropriately with respect to the lattice structure of the polarizer material. Effectively, this results in a low probability for photons with the wrong polarization to pass. Nevertheless, the whole process is unitary.
 
  • #59
CharlesDarwin said:
This is the "collapse" of the wave function, neither more nor less
That is not right.
The quantum mechanical state "superposition of A and B" is different from the quantum mechanical state "It is A or B and we don't know which yet", and there is no classical analogy for the former.
 
  • Like
Likes richrf, David Lewis and Lord Jestocost
  • #60
rubi said:
Well, polarizers are understood quite well quantum mechanically in solid-state physics. What happens during an absorption is that photons are scattered into phonons, i.e. lattice vibrations, in the polarizer and the photon-phonon cross section is higher if the photon is polarized appropriately with respect to the lattice structure of the polarizer material. Effectively, this results in a low probability for photons with the wrong polarization to pass. Nevertheless, the whole process is unitary.

I'm willing to believe that the whole process is unitary if you include photons + phonons + the whole rest of the universe. But it's not a unitary transformation on photon states.
 

Similar threads

  • · Replies 59 ·
2
Replies
59
Views
7K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 18 ·
Replies
18
Views
3K
  • · Replies 20 ·
Replies
20
Views
5K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 71 ·
3
Replies
71
Views
7K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K