Is the collapse of a wave function deterministic or random?

In summary, Bell's theorem is a theorem in quantum mechanics that states that it is impossible to determine the state of a particle before it is measured, even if you know the wave function.
  • #1
Happiness
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Suppose I measure the position of a particle, and I find it to be at point C.

By deterministic, I mean if we know the wave function of the measuring instrument (and of course also the wave function of the particle before measurement) then we can, in principle, know that the particle is going to be at point C during the measurement.

And by random, I mean there is no way we can, in principle, know that the particle is going to be at point C.
 
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  • #2
It's random. Even if you know the exact wave function, it only tells you how likely it is for the particle to be measured at point C.
 
  • #3
Without the measurement being made, there is no position of the particle. However, there is one wrinkle to this. If the particle is one of an entangled pair of particles, and the position of its twin has been measured, then the position of this particle is known and the result of its position measurement is very predictable.

So in some cases we have enough information available to make a prediction.

But more generally, we do not have enough information collected - and in most cases we need to suspect that it would be impossible to assemble that information - making it effectively (if not also in principle) impossible.
 
  • #4
Can I say that since the measuring instrument is the cause of the collapse of the particle's wave function, the measuring instrument should contain information that tells us which state the particle's wave function is going to collapse to during measurement?
 
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  • #5
Happiness said:
Can I say that since the measuring instrument is the cause of the collapse of the particle's wave function, the measuring instrument should contain information that tells us which state the particle's wave function collapses to?
You cannot. That's one of the implications of Bell's theorem (google for it, or try this website maintained by our own @DrChinese).
 
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  • #6
Happiness said:
Suppose I measure the position of a particle, and I find it to be at point C.

By deterministic, I mean if we know the wave function of the measuring instrument (and of course also the wave function of the particle before measurement) then we can, in principle, know that the particle is going to be at point C during the measurement.

And by random, I mean there is no way we can, in principle, know that the particle is going to be at point C.

As far as the mathematics of quantum mechanics are concerned, it is random. There's no way it cannot be, as the theory is explicitly about the probability of a measurement having a given result - you take the wave function, you crank it through the math, and you end up with a probability (or an expectation value if you integrate the probabilities across all the possible results)... And then QM has told you all it's ever going to tell you. If you want more, you have to perform the measurement and find out if the particle is there or not.
 
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  • #7
Happiness said:
Can I say that since the measuring instrument is the cause of the collapse of the particle's wave function, the measuring instrument should contain information that tells us which state the particle's wave function collapses to?
Here's another experiment that illustrates what needs to be considered when determining where a particle lands.

A Mach-Zehnder interferometer is a fairly simple device that splits a laser beam and recombines it to form an interference pattern.
It's described here: https://web.phys.ksu.edu/vqmorig/tutorials/online/wave_part/
And shown here:
mach_zeh.gif

Once it's set up and running, it looks like this:
muster1.gif

Actually, with a red laser, the projection looks like this:
Newtons_rings_650nm_red_laser_light.jpg


The first thing to consider is this, not all of the photons coming out of the laser land in the same place - even though the target (the screen) isn't changing. So clearly something more than the target is involved.

Notice in particular that there are dark areas in the pattern where photons never go. Each photon interferes with itself so that when it lands on the screen, it can be anywhere except the darkest places.

In that first diagram, you will see that there is a path A and a path B. If I block path A, the result will be a solid red blur being projected onto the screen.
Now consider the photons that are landing where those dark bands used to be. The reason they are getting there is because path A is blocked. But they obviously didn't take path A, because if they did, they would have hit the block and would never have reached the screen. Instead they took path B. They reached their location on the screen because they could have hit the block but didn't. So even things that didn't happen can affect where the particle is detected.
 
  • #8
Nugatory said:
You cannot. That's one of the implications of Bell's theorem (google for it, or try this website maintained by our own @DrChinese).

Bell's theorem shows that a particle did not have a determinate position before the measurement, but it does not rule out the possibility that the measuring instrument causes the collapse of a particle's wave function in a deterministic way.
 
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  • #9
Happiness said:
Bell's theorem shows that the particle did not have a determinate position before the measurement, but it does not rule out the possibility that the measuring instrument causes the collapse of a particle's wave function in a deterministic way.
In what way would you distinguish "have a determinate position before the measurement" from "collapse of a particle's wave function in a deterministic way"?
 
  • #10
Heinera said:
In what way would you distinguish "have a determinate position before the measurement" from "collapse of a particle's wave function in a deterministic way"?

If a particle has a determinate position before the measurement, then it was somewhere even though we do not know where it was.

If the wave function of a particle collapses in a deterministic way, then it is possible to have a mechanism describing the collapse.
 
  • #11
Happiness said:
If a particle has a determinate position before the measurement, then it was somewhere even though we do not know where it was.

If the wave function of a particle collapses in a deterministic way, then it is possible to have a mechanism describing the collapse.
But if the wave function is known, and the mechanism describing the collapse is known (and determinate), what prevents me from deducing the position of the particle without actually doing the measurement?
 
  • #12
Heinera said:
But if the wave function is known, and the mechanism describing the collapse is known (and determinate), what prevents me from deducing the position of the particle without actually doing the measurement?

Because the particle did not have a determinate position before the measurement, provided it's pre-measurement wave function is not sharply peaked at any point. The particle exists more like a ripple on a water surface, but the measurement process collects all the energy of the ripple and places it at a determinate position, for example.
 
  • #13
Happiness said:
Because the particle did not have a determinate position before the measurement, provided it's pre-measurement wave function is not sharply peaked at any point. The particle exists more like a ripple on a water surface, but the measurement process collects all the energy of the ripple and places it at a determinate position, for example.

But what determines whether the collapse is to one of the possible results or another? There has to be something that that we can use, if we just knew what it was, to calculate the determined result of your hypothetical deterministic process. Where does that something fit in Bell's ##\lambda## variables that specify the state?

(Actually, I do believe that there is an intellectually coherent way for collapse to be deterministic... but it takes you all the way to superdeterminism. Bell hasn't left a lot room in between).

[Edit: If you're willing to accept the state of the other (distant, spacelike-separated) as part of the "measuring apparatus" you can construct a consistent but non-local deterministic theory. Without a specific candidate theory though, it's not going to be experimentally distinguishable from the randomness that's inherent in the mathematical formulation of QM]
 
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  • #14
Happiness said:
Because the particle did not have a determinate position before the measurement, provided it's pre-collapsed wave function is not sharply peaked at any point. The particle exists more like a ripple on a water surface, but the measurement process collects all the energy of the ripple and places it at a determinate position, for example.
And if this measurement process that "collects all the energy" is deterministic, then it is equivalent to the particle having a specific property before the measurement, as far as Bell's theorem is concerned.
 
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  • #15
Heinera said:
And if this measurement process that "collects all the energy" is deterministic, then it is equivalent to the particle having a specific property before the measurement, as far as Bell's theorem is concerned.

Bell's theorem shows that local realism is incompatible with quantum mechanics, but this is not what I'm asking.

A clearer phrasing of my question would be as follows:
We know that the wave function of a particle evolves in a deterministic way according to the Schrodinger equation when the particle is not being measured. Suppose I measure the position of a particle, and I find it to be at point C. We know that its wave function evolves to one that is sharply peaked at point C during the measurement. Is such evolution of the wave function deterministic or random?
 
  • #16
Happiness said:
Bell's theorem shows that local realism is incompatible with quantum mechanics, but this is not what I'm asking.

A clearer phrasing of my question would be as follows:
We know that the wave function of a particle evolves in a deterministic way according to the Schrodinger equation when the particle is not being measured. Suppose I measure the position of a particle, and I find it to be at point C. We know that its wave function evolves to one that is sharply peaked at point C during the measurement. Is such evolution of the wave function deterministic or random?
So far, that is a matter of personal opinion. QM, at its current development, does not address this. To my knowledge, there is no experiment that has been proposed that would differentiate between a truly random result and one that is determined by the non-local environment in a deterministic way.

I have argued in other threads that if the result is truly random, then the decision is being made by adding information to the universe. Something that is inconsistent with QM. However, I have not been persuasive.
 
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  • #17
Happiness said:
If the wave function of a particle collapses in a deterministic way, then it is possible to have a mechanism describing the collapse.

Collapse is not part of the QM formalism, only some interpretations.

The answers to the questions you are asking depends entirely on interpretation.

Pick an interpretation, any interpretation:
https://en.wikipedia.org/wiki/Interpretations_of_quantum_mechanics

Once you have done that then answering your questions will be much easier.

Thanks
Bill
 
  • #18
Also, please don't choose Bohm or the consciousness thing. :smile:
 
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  • #19
Happiness said:
The particle exists more like a ripple on a water surface,

That's an interpretation you are putting on it.

The QM formalism is silent on what's going on when not observed.

As I said in a previous post, pick an interpretation then answering your questions may be possible. The QM formalism is silent on many things so you must pick an actual interpretation to ask meaningful questions.

Thanks
Bill
 
  • #20
TESL@ said:
Also, please don't choose Bohm or the consciousness thing. :smile:

Bohm's OK - but this conciousness thing really annoys me. Still its a legit interpretation and can be chosen for illustrative purposes if that's the OP's thing.

Thanks
Bill
 
  • #21
bhobba said:
Collapse is not part of the QM formalism, only some interpretations.

The answers to the questions you are asking depends entirely on interpretation.

Pick an interpretation, any interpretation:
https://en.wikipedia.org/wiki/Interpretations_of_quantum_mechanics

Once you have done that then answering your questions will be much easier.

Thanks
Bill

What does it mean by the wave function never collapses in some interpretations? It seems like all interpretations have to agree that the wave function collapses but may disagree on the interpretation and the ontology of the collapse. By collapse, I mean the evolution of the wave function from one that is spread out in space to one that is sharply peaked at a point during a measurement. Some interpretations may argue that the collapse of the wave function is not due to a physical change in the system but only due to a change in the information of the system available to an observer, but they still cannot deny that the wave function collapses. Hence, the collapse still needs to be addressed regardless of the interpretation one takes.
 
  • #22
Happiness said:
What does it mean by the wave function never collapses in some interpretations? It seems like all interpretations have to agree that the wave function collapses but may disagree on the interpretation and the ontology of the collapse. By collapse, I mean the evolution of the wave function from one that is spread out in space to one that is sharply peaked at a point during a measurement.

It means that a measurement that does not destroy what's being measured is, in some interpretations, a state preparation procedure. This does away with the concept of collapse that is supposed to instantaneously change the state. State and state preparation procedure are, in those interpretations, synonymous. It also means that collapse never happens in MW. There are probably other ways to do away with it but can't think of them off the top of my head.

Thanks
Bill
 
  • #23
bhobba said:
It means that a measurement that does not destroy what's being measured is, in some interpretations, a state preparation procedure. This does away with the concept of collapse that is supposed to instantaneously change the state. State and state preparation procedure are, in those interpretations, synonymous. It also means that collapse never happens in MW. There are probably other ways to do away with it but can't think of them off the top of my head.

Thanks
Bill

A measurement that does not destroy what's being measured would be a measurement done on a particle whose wave function is already peaked at a point, so naturally there isn't a collapse (or there is but a trivial one; it just evolves to the same wave function). But what about a measurement done on a particle whose wave function is spread out. Shouldn't there be a collapse?

Does MW mean many-worlds interpretation? How does it do away with the collapse? Even if all the possible outcomes are realized but in different parallel worlds, we still observe only one outcome and hence the wave function collapses.

Wikipedia: "In many-worlds, the subjective appearance of wavefunction collapse is explained by ..." So even many-worlds interpretation does not deny that the wave function collapses.
 
  • #24
Happiness said:
A measurement that does not destroy what's being measured would be a measurement done on a particle whose wave function is already peaked at a point\

That's incorrect. In the double slit experiment the slit does a position measurement on a particle without an actual position.

Happiness said:
Does MW mean many-worlds interpretation? How does it do away with the collapse?

It interprets the elements of a mixed state after decoherence as separate worlds so no change in the wave function happens.

Happiness said:
Wikipedia: "In many-worlds, the subjective appearance of wavefunction collapse is explained by ..." So even many-worlds interpretation does not deny that the wave function collapses.

You do understand the difference between actual and appearance don't you?

Thanks
Bill
 
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  • #25
bhobba said:
That's in correct.
It interprets the elements of a mixed state after decoherence as separate worlds so no change in the wave function happens.
You do understand the difference between actual and appearance don't you?

Thanks
Bill

Could you explain more?
 
  • #26
Happiness said:
Could you explain more?

Which part?

Thanks
Bill
 
  • #27
bhobba said:
Which part?

Thanks
Bill

I am not asking whether the collapse of a wave function is actual or apparent. It seems that there are some interpretations that argue that the collapse is apparent and not actual. It seems that in all interpretations, the collapse is either actual or apparent or some of them are agnostic about it. So are you saying there are interpretations where the collapse is apparent or are you saying there are interpretations where there is no collapse, not even apparently?
 
  • #28
Happiness said:
I am not asking whether the collapse of a wave function is actual or apparent. It seems that there are some interpretations that argue that the collapse is apparent and not actual. It seems that in all interpretations, the collapse is either actual or apparent or some of them are agnostic about it. So are you saying that there are interpretations where the collapse is apparent or are you saying there are interpretations where there is no collapse, not even apparently?

Ok you need to understand what collapse is.

Its the following idea. The systems state deterministically changes according to Schroedinger's equation. When an observation happens it instantaneously and randomly changes to a another state.

We have interpretations that refute pretty much any or all parts of that.

1. The ensemble interpretation doesn't have an instantaneous state change - instead all you have done is prepare the system differently - there is no discontinuous change:
https://en.wikipedia.org/wiki/Ensemble_interpretation

2. Many worlds has no change at all in the state, everything continues to evolve according to Schroedinger's equation:
https://en.wikipedia.org/wiki/Many-worlds_interpretation

3. There is another called Decoherent Histories that doesn't even have observations - instead it has the concept of history. It views QM as the stochastic theory of histories.
https://www.math.rutgers.edu/~oldstein/papers/qts/node2.html
http://quantum.phys.cmu.edu/CQT/index.html

I linked to a table before that examined the ideas of various interpretations.

If you want to ask the kind of questions you are asking you must first specify an interpretation.

Thanks
Bill
 
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  • #29
Happiness said:
I am not asking whether the collapse of a wave function is actual or apparent. It seems that there are some interpretations that argue that the collapse is apparent and not actual. It seems that in all interpretations, the collapse is either actual or apparent or some of them are agnostic about it. So are you saying there are interpretations where the collapse is apparent or are you saying there are interpretations where there is no collapse, not even apparently?
For example, you make a position measurement by having a photon strike a vidicon tube. The photon could have struck anywhere on the measuring surface - but with collapse, it has "chosen" a spot. Without collapse, the detection surface of the vidicon tube is now in a superposition of all possible detection locations. Next, an electron will be ejected from the surface and will accelerate towards the display face. With collapse, that will be a single photon. Without collapse, the vacuum section of the vidicon tube is filled with a superposition of electrons representing all possible measurements. Light is then emitted from the back of the vidicon tube and is focused by the retina of the observer. With collapse, only specific parts of the retina are activated, corresponding to where the original photon "chose" to land. Without collapse, the retina is in a superposition of states corresponding to many possible measurements. The human observer then becomes "conscious" of the photon position. With collapse, that will result in a specific revelation related to the original photon landing spot. Without collapse, the observers brain is in a superposition of many conscious states. Finally, the observer decides to report the result to his colleague. Let's say that event causes the entire wave function to collapse. So finally, we have a particular landing position, a particular electron, a particular retina activity, a particular conscious revelation, and a particular vocal report.

It should be clear from this that it doesn't matter when the collapse occurs or even if it doesn't occur. The final result is the same. But remember, these wave functions are not like the Multi World Interpretation. They are Schrodinger wave functions with all the superpositions interacting with each other. If we performed the Schrodinger Cat experiment, we would never expect to see a live cat that had eaten its dead superposition. So as we delay the "collapse" and the result expands into the macro world, something keeps us from observing self-eating cats.
 
  • #30
.Scott said:
It should be clear from this that it doesn't matter when the collapse occurs or even if it doesn't occur. The final result is the same.

But if there is no collapse, then the different eigenstates superimpose and produce an interference pattern (say, of a double-slits experiment). If the wave function collapses to a single eigenstate, then the interference pattern is destroyed. So the final result is different.
 
  • #31
Happiness said:
But if there is no collapse, then the different eigenstates superimpose and produce an interference pattern (say, of a double-slits experiment). If the wave function collapses to a single eigenstate, then the interference pattern is destroyed. So the final result is different.
It would mean that you're in a superposition of conscious states. How would you know that? Is there any experiment that can differentiate when the collapse occurs? The apparent lack of self-eating cat suggests that many possibilities are lost as the wave function involves more and more of the macroscopic world. But even that does not suggest that a full collapse ever happens.
 

1. What is the collapse of a wave function?

The collapse of a wave function is a phenomenon in quantum mechanics where a particle's wave function, which describes its possible states, is reduced to a single state when it is measured or observed.

2. Is the collapse of a wave function deterministic or random?

This is a highly debated topic in the field of quantum mechanics. Some scientists believe that the collapse is a deterministic process, meaning that the outcome of the measurement can be predicted with certainty. Others argue that it is a random process, and the outcome cannot be determined beforehand.

3. What evidence supports the deterministic view?

One of the main pieces of evidence supporting the deterministic view is the fact that the Schrödinger equation, which describes the evolution of a wave function, is a deterministic equation. This means that if the initial conditions are known, the future state of the system can be predicted with certainty.

4. What evidence supports the random view?

One of the main pieces of evidence supporting the random view is the phenomenon of quantum superposition, where a particle can exist in multiple states simultaneously. This suggests that the outcome of the collapse is not predetermined, and the particle's state is only determined when it is measured or observed.

5. Can the collapse of a wave function be explained by current scientific theories?

No, the collapse of a wave function is still a mystery in the field of quantum mechanics. While there are different interpretations and theories attempting to explain it, there is no consensus among scientists. It remains one of the most intriguing and debated topics in physics.

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