I Where is the quantum system prior to measurement?

[Lynch101]

We're in agreement on some key points here, particularly with regard to certain things being interpretation dependent. But, if we unpack some of your statements here, we might be able to find agreement.

1) Statements about what a system must do only make sense to me with respect to some specific interpretation. The orthodox interpretation (basically Copenhagen) is slightly agnostic at this point, but not completely.

It is the agnosticism that would render it incomplete. We can unpack some of what you say to explore in what sense it is agnostic and therefore, potentially, incomplete.

A beam of light in an interferometer can travel on multiple distinct paths from the source to the detector, and claiming that a photon in the beam must have traveled on some speficic of those distinct paths is simply wrong with respect to the orthodox interpretation.

Let's unpack the idea that the system 'can travel on multiple distinct paths'. I can see two ways of interpreting this:
1) There are multiple distinct paths that the system can travel and it travels on one of those. This would imply the system has a definite position and follows one single path.

2) There are multiple paths and the system travels along more than one simultaneously. This would seem to necessitate some form of physical collapse.

By my reasoning, either 1 or 2 must be true. Remaining agnostic on which it is would render an interpretation incomplete.

Already talking of "a photon" is wrong, because photons don't have individuality. The photons in the beam are indistinguishable (even that word is too weak, they are inseparable) from one another.

We don't need to talk about 'photons', we can talk more generally about any system whatsoever with any characteristics whatsoever. If it operates in 3D space then there are certain rules it has to follow.

2) Could you please stop to damage the tricky word "complete" and stop to associate it to unclear concepts like "physical reality". And how can you extract anything from such an unclear concept, like that it would include something definitive.

I am referencing the EPR paper titled, 'Can quantum mechanical description of physical reality be considered complete?'.

4) Even so it is an interesting question whether the (minimal) statistical interpretation is complete, the result of an investigation into whether it is or not would be more convincing, without the impression that the words preceeding the "therefore" were biased from the start.

If we think in terms of 3D space and the basic rules that apply to traveling from one region of 3D space to another, and then consider the agnosticism of the minimal statistical interpretation, we arrive at the conclusion that it is incomplete. By my reasoning.

 

[Lynch101]

Space might be transcendental in this context, but you are positing a thing moving in it, distinct from the preparation and the measurement outcome.

The nature of space doesn't really matter here, as long as it can be represented 3 dimensionally.

We can create a graphical 3 dimensional model. We can then represent the the experiment within this graphical representation, in accordance with these 3 dimensions. The preparation device will have a position in one 3D region while the measurement apparatus will have a position in another, spatially separated region.

If something starts in the region of the preparation device and ends up in the region of the measurement device, how does it get there?

By my reasoning, it must traverse a path through the intervening 3D region. We can discard our intuitive ideas about the specific path it takes, but it must take a unique path through that region. That unique path could have it in multiple places at once, it could be everywhere in the finite 3D region, but it must travel a unique path through that space. Remaining agnostic on which path it takes would leave us with an incomplete description.

 

[Morbert]

If something starts in the region of the preparation device and ends up in the region of the measurement device, how does it get there?

You are again supposing the underlying reality can be made intelligible by concepts like a definite path. I think interpretations like consistent histories can help make this kind of intuition sharp and reliable, but a hardcore Copenhagenist defending themselves against Ballentine's charges would not necessarily grant you this level of intelligibility.

 

[gentzen]

Let's unpack the idea that the system 'can travel on multiple distinct paths'. ...

2) There are multiple paths and the system travels along more than one simultaneously. This would seem to necessitate some form of physical collapse.

Well, it can travel along more than one path in the othodox interpretation, and there is a collapse postulate in that interpretation. But I neither see why that collapse has to be a physical collapse, nor why a collapse would have to be present in any interpretation allowing this.

We don't need to talk about 'photons', we can talk more generally about any system whatsoever with any characteristics whatsoever.

We can talk of photons, electrons, atoms, ions, or molecules. The fact that things can be indistinguishable/inseparable remains, and any reasoning trying to negate this fundamental truth risks being inapplicable in discussions about quantum physics.
Maybe try to appreciate some of the consequences of that fact, like Fermi-Dirac statistics, and Bose-Einstein statistics. And also why insisting on a single continuous path with definite a position at all times would be incompatible with such inseparability.

I am referencing the EPR paper titled

Well, that paper presents a paradox. Using a paradox to make definite conclusions is tricky business. The irony is that Bohr loved paradoxes, and Einstein was great at inventing paradoxes. But Bohr's resolutions of Einstein's paradoxes were often just as disappointing as Alexander the Great slicing the Gordian know instead of untying it. I think Einstein's paradoxes deserved better than Bohr's resolutions.

then consider the agnosticism of the minimal statistical interpretation, we arrive at the conclusion that it is incomplete. By my reasoning.

Your reasoning and your conclusion are too trivial. I tried to explain before how such overly trivial reasoning can have negative impact. The question whether the minimal statistical interpretation is incomplete is an interesting and subtle question. It deserves better than a trivial misunderstanding of what is meant by being complete.

And as I said above, Einstein's paradoxes would have deserved better too. And thanks to Bell, at least one of them also got what it deserved. Demystifier has a paper that tries to do justice to another one of Einstein's paradoxes.

 

[Lynch101]

You are again supposing the underlying reality can be made intelligible by concepts like a definite path. I think interpretations like consistent histories can help make this kind of intuition sharp and reliable, but a hardcore Copenhagenist defending themselves against Ballentine's charges would not necessarily grant you this level of intelligibility.

No, I'm saying that if the system is operating in 3 dimensions then there are certain rules that apply to it. Taking a unique* path through the 3D region between the devices is one such rule.

Remaining agnostic on the path taken would render the description incomplete, by definition.

*it doesn't have to be our intuitive idea of a path which is a function of a single, well-defined value for position,

 

[hutchphd]

*it doesn't have to be our intuitive idea of a path which is a function of a single, well-defined value for position,

? Sorry, what then is a path?

 

[Lynch101]

Well, it can travel along more than one path in the othodox interpretation, and there is a collapse postulate in that interpretation. But I neither see why that collapse has to be a physical collapse, nor why a collapse would have to be present in any interpretation allowing this.

Again, we have to unpack what is meant by, 'travel along more than one path in the othodox interpretation'.

The 'physical reality' that EPR are referring to is nothing more than the experimental set-up in the lab, as opposed to the mathematical representation of it. The physical preparation device occupies a 3D region which we can represent graphically, as does the measurement apparatus. The physical preparation device prepares a physical system which interacts with the physical measurement apparatus. For something to get from the physical preparation device to the physical measurement device it must take a path through the intervening 3D region in the 'physical reality'.

If it takes more than one path through the 3D space and arrives at the measurement device, we should have more than one detection event, but we don't. We only have one. Therefore, the physical system which took multiple paths through the 3D region of 'physical reality' must physically collapse to a single, well-defined position.

We can talk of photons, electrons, atoms, ions, or molecules.

We can, but we don't need to. We can talk even more generally.

insisting on a single continuous path with definite a position at all times would be incompatible with such inseparability.

OK, we're obviously talking past each other here because I am not insisting on a 'continuous path with definite a position at all times'. I have been at pains to try and emphasise that is not what I am talking about.

I am talking about a unique path/route, but that unique path/route can be a combination of multiple 'continuous path with definite position at all times' (as you have mentioned previously). It might be more helpful to call it a 'route' for the purpose of this point.

If we imagine the various possible 'continuous path with definite position at all times'. Let's call them:
Path1
Path 2
Path 3

The unique route taken by the system could be a combination of the different paths:
Path 1 + Path 2
Path 1+ Path 3
Path 2 + Path 3
Path 1 + Path 2 + Path 3

It must take some route through the 3D space to get from the preparation device to the measurement apparatus. Remaining agnostic on which route is taken would render an interpretation incomplete, which is what the statistical interpretation appears to do.

Well, that paper presents a paradox. Using a paradox to make definite conclusions is tricky business. The irony is that Bohr loved paradoxes, and Einstein was great at inventing paradoxes. But Bohr's resolutions of Einstein's paradoxes were often just as disappointing as Alexander the Great slicing the Gordian know instead of untying it. I think Einstein's paradoxes deserved better than Bohr's resolutions.

I have read a few accounts which would agree with you on that point.

But, just to re-iterate the point. The 'physical reality' that EPR are referring to is simply the experiment which takes place in the physical world, as opposed to the mathematical description of it.

 

[Lynch101]

? Sorry, what then is a path?

The path taken by a quantum system could be a multi-valued path. It could be the idea of the system going through two slits instead of just one.

 

[hutchphd]

The unique route taken by the system could be a combination of the different paths:
Path 1 + Path 2
Path 1+ Path 3
Path 2 + Path 3
Path 1 + Path 2 + Path 3

Feynman says it is the sum of all available paths (modulated by the path integral of the action). So you are saying what?

.

 

[gentzen]

If it takes more than one path through the 3D space and arrives at the measurement device, we should have more than one detection event, but we don't. We only have one. Therefore, ...

OK, we're obviously talking past each other here because I am not insisting on a 'continuous path with definite a position at all times'. I have been at pains to try and emphasise that is not what I am talking about.

I am talking about a unique path/route, but that unique path/route can be a combination of multiple 'continuous path with definite position at all times' (as you have mentioned previously).

For me, your arguments give me the impression that you are simultaneously arguing that there would be some serious consequences if the system would take more than one path, and that simulataneously you are perfectly fine with it taking more than one path.

So maybe you hope that I will protest that you should decide for one position or the other. But if I would do so, you would say "see, similarly the system must decide for one path or the other". So I won't protest, and just accept that this is the way you argue.

My protest therefore remains that you risk to damage the tricky word "complete", and that your reasoning and conclusions are too trivial.

 

[Lynch101]

Feynman says it is the sum of all available paths (modulated by the path integral of the action). So you are saying what?.

The sum of all available paths through the 3D region of 'physical reality' i.e. the 3D region in the physical experimental set-up?

If that is the case, then a physical collapse is required to explain why we only observe a single well-defined position. Failure to specify a unique path leaves us with an incomplete description.

 

[PeterDonis]

By 'the state of the system' I'm referring to (or trying to) 'every element of the physical reality' à la EPR.

You can't just wave your hands and say this. You need to show us in a specific model how "the state of the system" is represented. For example, in Bohmian mechanics, "the state of the system" is the wave function plus the positions of all particles.

If no model meeting your requirements exists, then you have no basis for any of the claims you have been making. Even in this forum, where the rules are somewhat looser than in the regular QM forum, you still have to have some valid basis for discussion other than your personal opinion or preference.

 

[Lynch101]

For me, your arguments give me the impression that you are simultaneously arguing that there would be some serious consequences if the system would take more than one path, and that simulataneously you are perfectly fine with it taking more than one path.

Nothing more serious than has already been postulated by collapse theories.

If the system takes more than one path simultaneously, we require physical collapse to account for the observation in a single, well-defined position. If the path has a well-defined position at all times we have:
1) Bohmian Mechanics
2) Many Worlds
3) [Insert other interpretation]

Remaining agnostic on this question renders an interpretation an incomplete description of 'the physical reality'.

So maybe you hope that I will protest that you should decide for one position or the other. But if I would do so, you would say "see, similarly the system must decide for one path or the other". So I won't protest, and just accept that this is the way you argue.

The system doesn't necessarily need to take a 'single valued path', however, it must take either a 'single-valued path' or a 'multi-valued path'. Remaining agnostic on this question, as the minimal statistical interpretation appears to do, renders it an incomplete description of 'the physical reality'

My protest therefore remains that you risk to damage the tricky word "complete", and that your reasoning and conclusions are too trivial.

That's fair enough. I am inclined to disagree on that point.

 

[Lynch101]

You can't just wave your hands and say this. You need to show us in a specific model how "the state of the system" is represented. For example, in Bohmian mechanics, "the state of the system" is the wave function plus the positions of all particles.

If no model meeting your requirements exists, then you have no basis for any of the claims you have been making. Even in this forum, where the rules are somewhat looser than in the regular QM forum, you still have to have some valid basis for discussion other than your personal opinion or preference.

Bohmian Mechanics and Many Worlds specify that the system has a well-defined position at all times. Collapse theories posit physical collapse. I'm simply saying that remaining agnostic on that question renders an interpretation incomplete as description of 'the physical reality', to use the words of EPR. Which the minimal statistical interpretation appears to do.

 

[vanhees71]

Feynman says it is the sum of all available paths (modulated by the path integral of the action). So you are saying what?

.

What Feynman or rather his path integral says that in non-relativistic (sic!) quantum mechanics the transition probability amplitude (or more formally the propagator) is schematically given by
$$G(t,x;t_0,x_0)=F \sum_{\text{paths}} \exp(\mathrm{i} S[q,\dot{q}]/\hbar).$$
The sum (or rather functional integral) runs over all paths in configuration space with fixed boundary points $q(t)=x$ and $q(t_0)=x_0$. It's equivalent to solving the time-dependent Schrödinger equation for the corresponding Green's function.

This tells you that in the general case there's no specific path the particle is taking. That's in full accordance with standard quantum mechanics. The path integral is anyway just one more different way to formulate orthodox quantum theory.

It also tells you that you get the classical trajectory as the dominating contribution, if $|S-S_{\text{cl}}|/\hbar$ is rapidly rising when the paths are deviating from the classical trajectory, because the classical trajectory is determined by the stationary point of the action functional, and then you can use the approximation of the steepest-descend method to approximately evaluate the path integral.

 

[PeterDonis]

Bohmian Mechanics and Many Worlds specify that the system has a well-defined position at all times.

Bohmian mechanics does, yes. But not MWI. MWI says that "the state of the system" is the wave function, period. That's all there is.

I'm simply saying that remaining agnostic on that question renders an interpretation incomplete as description of 'the physical reality', to use the words of EPR.

And this, by itself, is just a statement of opinion, even for EPR. Others might have different opinions. There is no way to resolve such a dispute, so arguing about it is rather pointless.

 

[Morbert]

No, I'm saying that if the system is operating in 3 dimensions then there are certain rules that apply to it. Taking a unique* path through the 3D region between the devices is one such rule.

Remaining agnostic on the path taken would render the description incomplete, by definition.

*it doesn't have to be our intuitive idea of a path which is a function of a single, well-defined value for position,

Again, the only system a physicist commits to is the preparation and the measurement outcome. You are supposing some additional process made intelligible by e.g. some physical state $\lambda$, distinct from the preparation $\rho$, which has a direct ontological interpretation at all times between the preparation and measurement.

 

[Lord Jestocost]

I'm simply saying that remaining agnostic on that question renders an interpretation incomplete as description of 'the physical reality', to use the words of EPR.

In case I understand you correctly, you are believing that a “complete” theory must provide some picturization as, for example: “… for something to get from the physical preparation device to the physical measurement device it must take a path through the intervening 3D region in the 'physical reality'.”

Why?

P. A. M Dirac in “THE PRINCIPLES OF QUANTUM MECHANICS” (third edition, page 10) :

"...the main object of physical science is not the provision of pictures, but is the formulation of laws governing phenomena and application of these laws to the discovery of new phenomena. If a picture exists, so much the better; but whether a picture exists or not is a matter of only secondary importance. In the case of atomic phenomena no picture can be expected to exist in the usual sense of the word 'picture', by which is meant a model functioning essentially on classical lines.“

 

[jbergman]

Bohmian Mechanics and Many Worlds specify that the system has a well-defined position at all times. Collapse theories posit physical collapse. I'm simply saying that remaining agnostic on that question renders an interpretation incomplete as description of 'the physical reality', to use the words of EPR. Which the minimal statistical interpretation appears to do.

I think there are some interesting questions here but I am not sure I agree with your framing of them in terms of complete and incomplete.

Really, what you are positing is that a complete theory must provide some physical explanation of the wave function outside of the context of measurements.

In the double slit experiment, we cannot "measure" whether a particle passes through one slit or both slits. We only know that if we measure the particle going through a slit then the interference pattern disappears.

So all we really know is that the wave function describes the probabilities we will measure for an ensemble of particles prepared in the same state.

Anything beyond that is speculation.

 

[Killtech]

In the double slit experiment, we cannot "measure" whether a particle passes through one slit or both slits. We only know that if we measure the particle going through a slit then the interference pattern disappears.

Out of curiosity, is that statement formally true?

Assume $|L>$ be the state of an particle passing left slit and $|R>$ the right one. Then the projection operator onto the state $\frac {1} {\sqrt 2} (|L> +|R>)$ suffices the axiomatic requirements for an observable. Therefore we can (at least formally) measure that observable and thus in theory give an answer within the framework of the theory.

 

[jbergman]

Out of curiosity, is that statement formally true?

Assume $|L>$ be the state of an particle passing left slit and $|R>$ the right one. Then the projection operator onto the state $\frac {1} {\sqrt 2} (|L> +|R>)$ suffices the axiomatic requirements for an observable. Therefore we can (at least formally) measure that observable and thus in theory give an answer within the framework of the theory.

I believe you are correct. In other words, we can create an observable to measure whether or not the photon went through both slits or not.

Peter Shor discusses that here, https://physics.stackexchange.com/a/6861

 

[PeterDonis]

we can create an observable to measure whether or not the photon went through both slits or not.

That's not what the given observable measures. It measures whether the photon went through both slits in phase, or out of phase. The orthogonal state is $\frac{1}{\sqrt{2}} \left( \ket{L} - \ket{R} \right)$, so a "yes" measurement on the given observable means "went through both slits in phase" and a "no" measurement means "went through both slits out of phase". Neither one means "went through only one slit".

In other words, whether or not the photon "went through both slits" depends on what observable you choose to measure. If you choose to measure a "which-slit" observable, i.e., one in which a "yes" measurement means $\ket{L}$ and a "no" measurement means $\ket{R}$, then the photon went through just one slit. If you choose to measure the observable described by @Killtech, then the photon went through both slits.

 

[PeterDonis]

Peter Shor discusses that here, https://physics.stackexchange.com/a/6861

Shor is saying the same thing I said in post #142.

 

[vanhees71]

You can of course measure through which slit a single photon goes. However then you have to mark each photon somehow to imprint the corresponding which-way information.

One way to realize it is to start with a source of $\varphi=0$-polarized (where the photon momentum is assumed to be in $z$ direction and $\varphi$ is the angle of the polarization vector, which is in the $xy$-plane to the $x$ axis) photons and putting quarter-wave plates oriented $\pm \pi/4$ wrt. the $x$ axis. Then a photon going through the left slit is left-circular (helicity $h=+1$) and a photon going through the right slit is right-circular ($h=-1$) polarized. Thus indeed now you have an entanglement between the helicity of the photon and through which way it went:
$$|\psi \rangle=\frac{1}{\sqrt{2}} (|L,h=1 \rangle + |R,h=-1 \rangle).$$
The probability for registering the photon at a position $x$ on a far-distant screen is given by the correspondingly propagated state ket
$$|\psi' \rangle=\frac{1}{\sqrt{2}}(|\vec{k},h=1 \rangle + \exp[\mathrm{i} \phi(x)]|\vec{k},h=-1 \rangle ).$$
Here $\vec{k}$ is the momentum of the photon if it's registered at position $x$ behind the screen and $\phi(x)=k x d/L$ the phase shift between a photon's probability amplitudes going through the left or right slit. Since now the photon states with helicities $\pm 1$ are perpendicular to each other there is no interference term between "going through the L or R slit", i.e., there's no two-slit interference pattern (only a single-slit interference pattern, not taken into account in this schematic treatment).

If you just don't put the quarter-wave plates at the slits, the state at the screen is
$$|\psi' \rangle=\frac{1+\exp(\phi(x))}{|1+\exp(\phi(x))|}|\vec{k}, \varphi=0 \rangle$$
and you get an interference term.

That's an example what Bohr called the complementarity between having which-way information and thus in some very loose sense "particle properties" (no two-slit interference pattern) or having no which-way information and ("wave properties") (two-slit interference pattern).

 

[Lynch101]

Bohmian mechanics does, yes. But not MWI. MWI says that "the state of the system" is the wave function, period. That's all there is.

Ah yes, my apologies. I was thinking that because MWI was a fully deterministic interpretation that it implied that particle had well-defined positions at all times, but MWI says that branching occurs upon measurement.

And this, by itself, is just a statement of opinion, even for EPR. Others might have different opinions. There is no way to resolve such a dispute, so arguing about it is rather pointless.

It's not simply a matter of opinion. It's the application of basic principles of 3D modeling to the experimental set-ups and making inferences/deductions about the implications.

If an interpretation doesn't conform to these basic principles then this tells us something about its compatibility with the 3D model.

 

[vanhees71]

But that's a different and in my opinion the only physically sensible statement: The position of quantum systems are only determined by experimental setups (macroscopic detectors). All you can say about the quantum system's position before using this setup to measure it all you know, given the quantum state, the probability distribution for detecting the quantum system at the location defined by this measurement apparatus.

An extreme example are single-photon Fock states: Since the photon itself has no position observable in the usual sense all you know about it being prepared in such a single-photon Fock state is the probability to measure it at a location determined by the photon detector (e.g., a CCD cam/pixel detector, where the position is defined by the pixels, also defining the spatial resolution, which is always finite).

 

[Lynch101]

Again, the only system a physicist commits to is the preparation and the measurement outcome. You are supposing some additional process made intelligible by e.g. some physical state $\lambda$, distinct from the preparation $\rho$, which has a direct ontological interpretation at all times between the preparation and measurement.

Physicists also commit to the propagation of causal influences at a finite speed, don't they?

Let's put the system itself to one side for a moment. We can try to add it back in at the end.

We can start by creating a 3 dimensional model, basically just a model with the XYZ axes. We can then represent the experimental set-up within that model i.e. the preparation device, the screen with the slits, and the measurement apparatus. For this model to be representative of 'the physical reality' i.e. the physical experimental set-up in the lab, there must be something corresponding to 'the slits' in the screen at the noumenlogical level.

In our 3D model we can represent the 3D region where the preparation device is, together with the spatially separated 3D region where the measurement apparatus is. We can attempt to represent everything else in the universe within the 3D model. Essentially, if something operates within 3D dimensions we can represent it in our model, since our model doesn't allow anywhere to hide in those 3 dimensions.

Identifying the 3D regions, corresponding to the measurement apparatus and the preparation device, in our model we can ask the question. If something/anything starts in the finite 3D region of the preparation device and ends up in the 3D region of the measurement device, how does it get there? Well, it could just instantaneously go from preparation device to measurement apparatus, however, our 'no FTL propagation' prohibits this.

So, if it can't instantaneously go from one 3D region to the other, it must propagate, with a finite speed in the intervening 3D region.

Thinking about our screen now and how we represent it in the 3D model. We can represent it as a line which acts as a barrier between the two regions. When we do this, according to our model, there is no way to get from one region to another. When we put 'slits' in the 'screen' there are now possible routes between the two regions.

Given that there is nowhere to hide in our 3D model, something which starts in one region and ends up in the other, must follow some unique path through the intervening 3D region.Now, where does our quantum system fit into this? If we remain agnostic on the unique route taken, then our 3D model cannot be complete. If we say that it does not take a unique route then it doesn't fit within our 3D model and it must be propagating in other dimensions or instantaneously from one region to the other.

 

[Lynch101]

In case I understand you correctly, you are believing that a “complete” theory must provide some picturization as, for example: “… for something to get from the physical preparation device to the physical measurement device it must take a path through the intervening 3D region in the 'physical reality'.”

Why?

P. A. M Dirac in “THE PRINCIPLES OF QUANTUM MECHANICS” (third edition, page 10) :

"...the main object of physical science is not the provision of pictures, but is the formulation of laws governing phenomena and application of these laws to the discovery of new phenomena. If a picture exists, so much the better; but whether a picture exists or not is a matter of only secondary importance. In the case of atomic phenomena no picture can be expected to exist in the usual sense of the word 'picture', by which is meant a model functioning essentially on classical lines.“

The object of physical science may not be to draw pictures, however, we can still draw pictures and ask how the physical world conforms to those pictures - and make deductions/inferences accordingly.

If we model the universe in 3 dimensions, and our model is complete, we should be able to represent everything in the universe in 3D. From this 3D model we can infer rules about how anything operating within 3 dimensions must behave. Adding a 'no FTL propagation' principle we can say, for anything - operating within 3 dimensions - to propagate (with a finite speed) from one 3D region to another it must follow some unique path through the intervening 3D region. This is just what a 3D picture says must be the case.

If we do not, or can not specify the unique route taken by something which starts in the 3D region of the preparation device and ends up in the 3D region of the measurement device then either our model is not a complete description of 'the physical reality' i.e. what is happening in the physical experimental set-up or, the system which propagates from the preparation device to the measurement apparatus does not do so in 3 dimensions.Note: this unique path does not have to conform to our intuitive ideas of the system having a single, well-defined value at all times. It could be a mutli-valued path, it could occupy the entire 3D region, or any other such unique path. Remaining agnostic on this is what renders a description incomplete.

 

[Lynch101]

I think there are some interesting questions here but I am not sure I agree with your framing of them in terms of complete and incomplete.

Really, what you are positing is that a complete theory must provide some physical explanation of the wave function outside of the context of measurements.

In the double slit experiment, we cannot "measure" whether a particle passes through one slit or both slits. We only know that if we measure the particle going through a slit then the interference pattern disappears.

It might be better to say that a complete 3D model must specify the unique path taken by the system from one spatially separated region to another. At the very least, it must allow that some unique path (through the intervening 3D region) is taken.

Remaining agnostic would render it an incomplete 3D model.

So all we really know is that the wave function describes the probabilities we will measure for an ensemble of particles prepared in the same state.

Anything beyond that is speculation.

We don't need to speculate about the rules of our 3D model.

Where something begins in one 3D region and ends up in another, spatially distant 3D region and where no FTL propagation is permitted, it must take some unique route through the intervening 3D region. Remaining agnostic on what route is taken renders a 3D model incomplete. Saying that no unique route is taken implies other dimensions.

The minimal statistical interpretation appears to remain agnostic.

 

[WernerQH]

If we do not, or can not specify the unique route taken by something which starts in the 3D region of the preparation device and ends up in the 3D region of the measurement device then either our model is not a complete description of 'the physical reality' i.e. what is happening in the physical experimental set-up or, the system which propagates from the preparation device to the measurement apparatus does not do so in 3 dimensions.

I admire your persistence. It may not be obvious to you, but ironclad logic loses its force when a flawed assumption is included. You have achieved reductio ad absurdum of the idea that quantum theory can be understood in terms of quantum "objects" (or what you call "systems"). Probably you'll never be able to make sense of quantum theory.