ftr
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So does TI says anything about which slit or slits. Or silent on the issue.
The C60 field goes through both slits, analogous to a classical electromagnetic field, and materializes at the screen in the form of individual C60 molecules.ftr said:So does TI says anything about which slit or slits. Or silent on the issue.
A. Neumaier said:The C60 field goes through both slits, analogous to a classical electromagnetic field, and materializes at the screen in the form of individual C60 molecules.
For the sake of comparison, let me tell what what standard Bohmian mechanics (BM) and instrumental Bohmian mechanics (IBM) say.vanhees71 said:So it says the same as the (minimal) standard interpretation...
The field goes through both slits. This has nothing to do with wave functions (in general there is no wave function but only a density operator).EPR said:If the wavefunction goes through both slits
They are not actualized, that's all.EPR said:what happens to the unactualized possibilities in the TI?
It was always enough to consider what is the case rather than what is just a possibility but then does not happen.EPR said:So it's another description - nice to have but not an interpretation per se.
If the C60 field can be thought as being spread out over a larger area (how large?) and during measurement contracts instantaneously to form a C60 molecule then this notion seems to replace the collapse of the wave function by the collapse of a field. Thereby this field is presumably a real thing, not just a mathematical construct. But if correct so far isn't this an unphysical notion?A. Neumaier said:The C60 field goes through both slits, analogous to a classical electromagnetic field, and materializes at the screen in the form of individual C60 molecules.
Has the TI two views, one where a complex molecule is a field and another one where a complex molecule is rigid?A. Neumaier said:Because 4 points are needed to fix a definite frame in space. Thus fixing the mean positions of 4 nuclei produces an approximate rest frame of the C60 molecule. Because such a molecule is quite rigid, it determines the position of all nuclei up to a tiny uncertainty.
In the TI, both fields and collapse are physical. But in general, collapse is described not by jumping into an eigenstate but by the output of an appropriate quantum instrument.timmdeeg said:If the C60 field can be thought as being spread out over a larger area (how large?) and during measurement contracts instantaneously to form a C60 molecule then this notion seems to replace the collapse of the wave function by the collapse of a field. Thereby this field is presumably a real thing, not just a mathematical construct. But if correct so far isn't this an unphysical notion?
No. the TI is a single interpretation. But C60 can be modeled by standard quantum mechanics in different details and in different situations, leading to different descriptions.timmdeeg said:Has the TI two views, one where a complex molecule is a field and another one where a complex molecule is rigid?
But doesn't the instantaneous collapse of a physical field (to form a molecule on the screen) violate Special Relativity?A. Neumaier said:In the TI, both fields and collapse are physical. But in general, collapse is described not by jumping into an eigenstate but by the output of an appropriate quantum instrument.
My question in #734 was related to your statement "It moves along a fuzzy world tube centered around the path given by the q-expectations of the position, with a width given approximately by the square root of the sum of the q-variances." Which I understood such that the rigid C60 "moves along a fuzzy world tube ..." before it is materialized at the screen. Thanks for clarifying that now.A. Neumaier said:The description of C60 as a reasonable rigid molecule is appropriate for a C60 molecule at the surface of a screen (as measured in double slit experiments). Both descriptions are therefore needed to analyze double slit experiments.
Well, behind a double slit, it changes its shape due to diffraction to a union of two fuzzy spheres centered on the two slits. Moreover this affects only the wholesale shape, not the internal shape. Local and nonlocal qualities coexist.timmdeeg said:My question in #734 was related to your statement "It moves along a fuzzy world tube centered around the path given by the q-expectations of the position, with a width given approximately by the square root of the sum of the q-variances." Which I understood such that the rigid C60 "moves along a fuzzy world tube ..." before it is materialized at the screen. Thanks for clarifying that now.
I must say I do not agree. If QFT predicts that a 'collision' between succesive molecules and the slits produces an interference pattern - what is incoherent about that ?EPR said:There is no coherent explanation of the double slit experiment. If assumptions of how the world is and how it works is true, the double slit shouldn't produce the patterns it does. This is the weakest point in quantum physics and the topic of many many thousands of unresolved debates. It is where literally all interpretations fail and possibly the biggest mistery of nature at this time.
QFT is the best and the only coherent 'interpretation' of reality to date. By FAR. No question about it. Though it contains in itself the only mistery - the measurement problem.Mentz114 said:I must say I do not agree. If QFT predicts that a 'collision' between succesive molecules and the slits produces an interference pattern - what is incoherent about that ?
EPR said:There is no coherent explanation of the double slit experiment. If assumptions of how the world is and how it works is true, the double slit shouldn't produce the patterns it does. This is the weakest point in quantum physics and the topic of many many thousands of unresolved debates.
EPR said:QFT was the best and most coherent description of the world when i started researching this topic 15 years ago. It is still by far the best scientific attempt to explain the world without noise and nonsense. Backed up by thousands successful experiments and established facts. Hardcore science at its best. Can't ask for more.
One of them says 'the most coherent description of reality', while the other says 'there is no coherent explanation of the double slit experiment'.PeterDonis said:These two statements of yours appear inconsistent. Which of them do you really mean to say?
EPR said:One of them says 'the most coherent description of reality', while the other says 'there is no coherent explanation of the double slit experiment'.
EPR said:one of them is an almost complete worldview(sans GR and gravity), the other is the final(though still far away) obstacle to understanding the relationship between the classical and quantum world
PeterDonis said:Unless you are claiming that double slit experiments are not real, having a coherent explanation of reality should include having a coherent explanation of the double slit experiment.
No, QFT does not solve the MP. However it already provides a picture of reality.Either QFT solves this problem or it doesn't. If it does, then the obstacle you describe has been overcome. If it doesn't, then you don't have a coherent description of reality, since gravity is part of reality.
So, again, which is it?
EPR said:No, QFT does not solve the MP.
EPR said:However it already provides a picture of reality.
The so called world is a collection of fields that produce, 'create'(okay i will back off slightly here) and substitute that term with the more acceptable term - 'emerge' a classical world at the classical limit.
EPR said:Not all of reality.
I have googled for W. Sandhas but not sure which paper describes the method. Can you point to a specific paper, thanks.A. Neumaier said:The description of C60 as a field is appropriate for C60 beams (as prepared in double slit experiments); these are described by a current (constructible for arbitrary bound states according to a method due to Sandhas).
ftr said:I have googled for W. Sandhas but not sure which paper describes the method. Can you point to a specific paper, thanks.
The nonlocality of the thermal interpretation is a direct consequence of quantum field theory, hence as consistent with fundamental Lorentz covariance as quantum field theory itself. Thus provably in space-time dimensions 2 (quantum wires) and 3 (quantum surfaces), and empirically in space-time dimension 4.Demystifier said:@A. Neumaier I have one question for you. The thermal interpretation is an ontological interpretation, so it must be described by a nonlocal theory, as the Bell theorem implies. Is this fundamental nonlocality consistent with fundamental Lorentz covariance? Or does it mean that Lorentz covariance of QFT is emergent, rather than fundamental?
Nonlocal = dependent on more than one space-time position (which can be arbitrarily far apart in space).vanhees71 said:I'm a bit puzzled by what you define as "local" vs. "nonlocal". Why do you consider the (non-observable) n-point functions as "non-local"?
Yes, and there are also the unordered correlations corresponding to Wightman n-point functions.vanhees71 said:They are given by something like (for a scalar self-adjoint field as the most simple example)
$$G^{(n)}(x_1,\ldots,x_2)=\langle \mathcal{T} \hat{\phi}(x_1) \hat{\phi}(x_2) \cdots \hat{\phi}(x_n) \rangle,$$
where ##\mathcal{T}## is some "time-ordering prescription" (like time-ordering for vacuum QFT, contour-ordering for the most general case of real-time many-body QFT), and the expectation is meant as the trace with the stat. op.
I think I get it. You avoid Bell theorem by something I would call multi-ontology in a single world (as opposed to many-world interpretation, which could be called single-ontology in many worlds). For instance, let ##s_A## and ##s_B## be the ontological spins of two entangled particles, and let their ontological product be ##s_A\circ s_B##. In theories covered by the Bell theorem one hasA. Neumaier said:In the thermal interpretation, there are local distribution-valued beables, the q-expectations of fields, and nonlocal distribution-valued beables, the n-point correlation functions, q-expectations of products of fields at different points and their derivatives. These q-expectations are manifestly Lorentz covariant.
Demystifier said:let their ontological product be
An ontological quantity that in the classical limit is given by an ordinary product of two ontological quantities.PeterDonis said:What is an "ontological product"?
Demystifier said:An ontological quantity that in the classical limit is given by an ordinary product of two ontological quantities.
Informally, in the thermal interpretation, the whole is more than its parts, which makes perfect sense to me. Whereas Bell assumed that, as in classical n-particle mechanics, the complete description of the parts furnishes a complete description of the whole.Demystifier said:I think I get it. You avoid Bell theorem by something I would call multi-ontology in a single world (as opposed to many-world interpretation, which could be called single-ontology in many worlds). For instance, let ##s_A## and ##s_B## be the ontological spins of two entangled particles, and let their ontological product be ##s_A\circ s_B##. In theories covered by the Bell theorem one has
$$s_A\circ s_B=s_As_B$$
while in the thermal interpretation
$$s_A\circ s_B \neq s_As_B$$
The ontology with the inequality above does not make much sense to me, but that's essentially what the thermal interpretation, as far as I understood it, claims to be the case.
Then it's simply "non-local" because I make an experiment with two or more detectors at distant points in space, but that's trivial and has nothing to do with the complicated implications of what's usually meant by "non-locality" in the sense of "spooky actions at a distance", and then it's of course consistent with the standard interpretation of relativistic local QFT.A. Neumaier said:Nonlocal = dependent on more than one space-time position (which can be arbitrarily far apart in space).
This is the same notion of nonlocality that is used to decide whether a Lagrangian density is local or nonlocal. It is also the notion of nonlocality that is excluded in assumptions proving Bell inequalities, and is the kind of nonlocality established experimentally in long distance entanglement experiments.
In this sense, quantum fields and their q-expectations are local, but correlation functions are nonlocal.
An ordinary product of two ontological quantities is just an ordinary multiplication of numbers, as in classical physics. The thermal interpretation replaces this with something very non-classical (and in my opinion too weird to make sense ), which, in effect, can be expressed as a weird way of multiplication. It has its roots in the well-known multiplication of operators in QM, which also looks weird if one attempts to interpret operators as ontological. For that reason operators are not interpreted as ontological in any quantum interpretation I am aware of. But the thermal interpretation takes the expectation value of operator products as ontological, which can be expressed as a strange multiplication. This multiplication is mathematically well defined (because the product of operators is mathemicaly well defined), but it is very strange when interpreted ontologically, on which the thermal interpretation insists.PeterDonis said:What is "an ordinary product of two ontological quantities"? I only know how to multiply numbers and other mathematical objects; I don't know how to multiply "ontological quantities".
I reformulated it in this way to better understand the thermal interpretation in my own terms.A. Neumaier said:I don't understand your reformulation in terms of an ontological product which neither figures in Bell's work nor in mine.
OK, that's another way to express the fact that the Bell theorem does not apply to the thermal interpretation.A. Neumaier said:Informally, in the thermal interpretation, the whole is more than its parts. Whereas Bell assumed that the complete description of the parts furnishes a complete description of the whole.
"spooky actions at a distance" is not a physical phenomenon but the result of a poor interpretation.vanhees71 said:Then it's simply "non-local" because I make an experiment with two or more detectors at distant points in space, but that's trivial and has nothing to do with the complicated implications of what's usually meant by "non-locality" in the sense of "spooky actions at a distance", and then it's of course consistent with the standard interpretation of relativistic local QFT.
No, the expectation value of operator products cannot be expressed as a product of q-expectations, which are the beables of the parts! It gives truly additional beables - whence the whole has more properties than the parts.Demystifier said:But the thermal interpretation takes the expectation value of operator products as ontological, which can be expressed as a strange multiplication.
Yes, and a very intuitive one!Demystifier said:OK, that's another way to express the fact that the Bell theorem does not apply to the thermal interpretation.
Demystifier said:An ordinary product of two ontological quantities is just an ordinary multiplication of numbers, as in classical physics.
I think maybe Demystifier can do a write up on what is meant by "ontological" for various interpretations. He has been always good at summarizing contentious issues. Does "ontology" have a universal agreed upon meaning? or maybe I should open a thread.PeterDonis said:I think you are confusing the model with reality. Numbers are not "quantities"; they are things in our mathematical model.
A discussion of this question surely does not belong to this thread.ftr said:Does "ontology" have a universal agreed upon meaning? or maybe I should open a thread.
yes. This is what I was suggesting.A. Neumaier said:A discussion of this question surely does not belong to this thread.
ftr said:Does "ontology" have a universal agreed upon meaning? or maybe I should open a thread.
In ontological theories such as Bohmian mechanics of many worlds, if ##A## and ##B## are beables, then so is ##AB##. In thermal interpretation, it is not so. I find it too weird for my taste.A. Neumaier said:No, the expectation value of operator products cannot be expressed as a product of q-expectations, which are the beables of the parts! It gives truly additional beables - whence the whole has more properties than the parts.
Would you say that the thermal interpretation denies reductionism?A. Neumaier said:Yes, and a very intuitive one!
I would categorize all the interpretations into 3 categories:ftr said:I think maybe Demystifier can do a write up on what is meant by "ontological" for various interpretations. He has been always good at summarizing contentious issues. Does "ontology" have a universal agreed upon meaning? or maybe I should open a thread.
In the TI, the product of the q-expectations of A and B is a different beable than the q-expectation of the product AB. Nothing weird is involved.Demystifier said:In ontological theories such as Bohmian mechanics of many worlds, if ##A## and ##B## are beables, then so is ##AB##. In thermal interpretation, it is not so. I find it too weird for my taste.Would you say that the thermal interpretation denies reductionism?
In TI, the q-expectation does not have a statistical interpretation. It is a property of a single system, not of an ensemble of systems. From that perspective, I understand how a q-expectation of the product AB is calculated, but I can't understand what a q-expectation of the product AB is. Is there perhaps some analogy?A. Neumaier said:In the TI, the product of the q-expectations of A and B is a different beable than the q-expectation of the product AB. Nothing weird is involved.
Thanks. I hope to open a thread soon.Demystifier said:I would categorize all the interpretations into 3 categories:
1) Interpretations without ontology (most variants of Copenhagenish interpretations)
2) Interpretations with ontology but without primitive ontology (consistent histories, thermal interpretation)
3) Interpretations with primitive ontology (Bohmian, many worlds, objective collapse)
Primitive ontology is the fundamental ontological quantity to which all other ontological quantities can be reduced. In Bohmian mechanics it is particle positions of all particles in the Universe. In many worlds it is the wave function of the multiverse.
Demystifier said:In ontological theories such as Bohmian mechanics of many worlds, if ##A## and ##B## are beables, then so is ##AB##.