The cause I have in mind is of course a faster-than-light interaction, which of course is incompatible with orthodox relativistic QFT, which of course is why I have in mind an unorthodox relativistic QFT. The unorthodox relativistic QFT uses all the equations of orthodox QFT and makes the same measurable predictions, but the narrative is slightly different.vanhees71 said:Even if you agree with that, the cause is not a faster-than-light interaction, at least not within a local relativistic QFT, but it's due to the correlation described by entanglement.
There are no inconsistencies. You assume that only one interpretation (the orthodox one) is consistent with the undisputed equations, but that's wrong. There are many interpretations of quantum theory consistent with the equations of quantum theory.vanhees71 said:Well, but then you contradict the mathematical formulations. How can an interpretation make sense if it contradicts the mathematical foundations, and if all measurable predictions are the same what sense does it make to invent inconsistencies between interpretation on the one hand as well as the mathematical description and empirical facts?
https://www.physicsforums.com/threa...-concept-of-entanglement.1007463/post-6545856Demystifier said:Define "action"!
How can an interpretation claiming the existence of ftl interactions be consistent for a theory which excludes them in its mathematical formulation?Demystifier said:There are no inconsistencies. You assume that only one interpretation (the orthodox one) is consistent with the undisputed equations, but that's wrong. There are many interpretations of quantum theory consistent with the equations of quantum theory.
By using different terminology. Interaction means something else, not what you might have guessed. Just like non-local means something else, not the usual.vanhees71 said:How can an interpretation claiming the existence of ftl interactions be consistent for a theory which excludes them in its mathematical formulation?
By extending the set of interacting objects. Relativistic QFT excludes ftl interactions in a law for evolution of the state in the Hilbert space ##\psi##. But minimal relativistic QFT says nothing about other possible interacting objects ##\lambda## that are not given by ##\psi##. Bohmian interpretation is an extension of minimal relativistic QFT. It does not change the evolution of ##\psi##, but it makes a concrete proposal for ##\lambda## and postulates a nonlocal law for evolution of ##\lambda##. Since minimal and Bohmian QFT agree on equations for ##\psi##, and since minimal QFT says nothing mathematical about the evolution of ##\lambda##, there is no any mathematical contradiction between minimal and Bohmian QFT. The contradiction is only philosophical, because minimal QFT uses some philosophical arguments to argue that there is no ##\lambda## to begin with.vanhees71 said:How can an interpretation claiming the existence of ftl interactions be consistent for a theory which excludes them in its mathematical formulation?
Yes, and this is what makes this philosophy inclined topic so useless for science. You use the words not in their clear scientific meaning but distort them as long as it has no meaning anymore at all. Within the exact sciences one should say interaction when one means an interaction and correlation when one means correlation and should keep this strictly separated with a well-defined meaning. You save a lot of time for real discussions rather than defining again and again the same words.martinbn said:By using different terminology. Interaction means something else, not what you might have guessed. Just like non-local means something else, not the usual.
Standard QFT uses physical arguments and doesn't interoduce fictitious enigmatic entities called ##\lambda## in the first place. I guess you mean ##\lambda## as in Bell's original paper on his local deterministic HV models, and this is disproven by experiment. We can move on with new physics for at least 10-20 year now!Demystifier said:By extending the set of interacting objects. Relativistic QFT excludes ftl interactions in a law for evolution of the state in the Hilbert space ##\psi##. But minimal relativistic QFT says nothing about other possible interacting objects ##\lambda## that are not given by ##\psi##. Bohmian interpretation is an extension of minimal relativistic QFT. It does not change the evolution of ##\psi##, but it makes a concrete proposal for ##\lambda## and postulates a nonlocal law for evolution of ##\lambda##. Since minimal and Bohmian QFT agree on equations for ##\psi##, and since minimal QFT says nothing mathematical about the evolution of ##\lambda##, there is no any mathematical contradiction between minimal and Bohmian QFT. The contradiction is only philosophical, because minimal QFT uses some philosophical arguments to argue that there is no ##\lambda## to begin with.
Or schematically:
Minimal QFT: ##\psi## local, period.
Bohmian QFT: ##\psi## local, ##\lambda## nonlocal.
I mean Bell's ##\lambda## which can be either local or nonlocal. The nonlocal Bell's ##\lambda## is of course not disproven.vanhees71 said:I guess you mean ##\lambda## as in Bell's original paper on his local deterministic HV models, and this is disproven by experiment.
No, but there is nonrelativistic causal nonlocal theory for ##\lambda## which makes the same measurable predictions as relativistic local QFT.vanhees71 said:Is there any relativistic causal non-local theory for ##\lambda##?
So far nobody found computational advantages of Bohmian fields (BTW, there are examples of computational advantages of Bohmian particles), but it helps a lot to sharpen intuitions. In addition to offering a solution of the measurement problem, Bohmian fields offer a very simple solution of the problem of time in quantum gravity. (There is also a claim that it helps to solve the Boltzmann brain problem is cosmology, but I don't find it convincing.)Morbert said:Stepping away from the philosophy for a moment: Are there quantities Bohmian field theories can more readily compute? Or processes? I don't think a nonlocal skeleton ##\lambda## is automatically a bad idea, but does it sharpen any ambiguities or render some intuitions or computations more available?
I've tried to make it very simple in http://thphys.irb.hr/wiki/main/images/3/3d/QFound5.pdfvanhees71 said:How such a theory can make the same measurable predictions as relativistic local QFT is an enigma to me.
What is the physical counterpart of ##\lambda##?Demystifier said:By extending the set of interacting objects. Relativistic QFT excludes ftl interactions in a law for evolution of the state in the Hilbert space ##\psi##. But minimal relativistic QFT says nothing about other possible interacting objects ##\lambda## that are not given by ##\psi##. Bohmian interpretation is an extension of minimal relativistic QFT. It does not change the evolution of ##\psi##, but it makes a concrete proposal for ##\lambda## and postulates a nonlocal law for evolution of ##\lambda##. Since minimal and Bohmian QFT agree on equations for ##\psi##, and since minimal QFT says nothing mathematical about the evolution of ##\lambda##, there is no any mathematical contradiction between minimal and Bohmian QFT. The contradiction is only philosophical, because minimal QFT uses some philosophical arguments to argue that there is no ##\lambda## to begin with.
Or schematically:
Minimal QFT: ##\psi## local, period.
Bohmian QFT: ##\psi## local, ##\lambda## nonlocal.
In Bohmian mechanics it's a local beable such as particle positions or a field configuration. Note that local beables (ontic things with values at well defined points in space) have nonlocal interactions.martinbn said:What is the physical counterpart of ##\lambda##?
You need to write a dictionary. You said "By extending the set of interacting objects.", but particle positions are not physical object and cannot interact! Particles are objects that can interact. It seems that you uses phrases that should be used for the territory, but you use them for the map all the time. I know that you think I have a problem with nonlocality, but if everything was local I would have the same problem. It is just very hard to keep track of what is what.Demystifier said:In Bohmian mechanics it's a local beable such as particle positions or a field configuration. Note that local beables (ontic things with values at well defined points in space) have nonlocal interactions.
Did you try to read some other text (not written by me) on Bohmian mechanics? Did you have similar problems?martinbn said:You need to write a dictionary. You said "By extending the set of interacting objects.", but particle positions are not physical object and cannot interact! Particles are objects that can interact. It seems that you uses phrases that should be used for the territory, but you use them for the map all the time. I know that you think I have a problem with nonlocality, but if everything was local I would have the same problem. It is just very hard to keep track of what is what.
It's worse. I can ask you, but I cannot ask a text.Demystifier said:Did you try to read some other text (not written by me) on Bohmian mechanics? Did you have similar problems?
This is obviously a basic misinterpretation of the gauge-vector fields. These are of course not observables, because they don't fulfill the microcausality principle. Only gauge-independent quantities can be observables. To think there were an "ontology" of the vector potentials in gauge theories must be flawed and lead to wrong conclusions. Particularly it's clear that also the observable phase shifts in the Aharonov-Bohm effect are gauge invariant, because the magnetic flux entering them is gauge invariant and can be expressed with gauge-invariant fields, obeying the microcausality principle.Demystifier said:I've tried to make it very simple in http://thphys.irb.hr/wiki/main/images/3/3d/QFound5.pdf
You missed the point. Suppose that some hypothetical civilization only discovered electrodynamics in the Coulomb gauge and never discovered the gauge invariance. I claim that they would never observe any contradiction between theory and experiment. If you agree with that statement (and I don't see any reason why shouldn't you), then it should be obvious they would have a Lorentz and gauge non-noninvariant theory that agrees with experiments.vanhees71 said:This is obviously a basic misinterpretation of the gauge-vector fields. These are of course not observables, because they don't fulfill the microcausality principle. Only gauge-independent quantities can be observables. To think there were an "ontology" of the vector potentials in gauge theories must be flawed and lead to wrong conclusions. Particularly it's clear that also the observable phase shifts in the Aharonov-Bohm effect are gauge invariant, because the magnetic flux entering them is gauge invariant and can be expressed with gauge-invariant fields, obeying the microcausality principle.
An "ontology" is just a (mathematical) model in a certain sense, there is no need to draw premature conclusions. Using the vector potentials as model can indeed be dangerous, but the reasons are related to topology, not to the violation of Lorentz invariance. Gauge fixing always lead to valid local models, but topological obstructions often prevent getting a valid global model from such local models.vanhees71 said:To think there were an "ontology" of the vector potentials in gauge theories must be flawed and lead to wrong conclusions.
When you ask me, does it actually help?martinbn said:It's worse. I can ask you, but I cannot ask a text.
If they discovered (classical or quantum) electrodynamics they'd also have discovered gauge invariance, because electrodynamics makes only mathematical sense as a gauge theory, let alone its success in describing all electromagnetic phenomena.Demystifier said:You missed the point. Suppose that some hypothetical civilization only discovered electrodynamics in the Coulomb gauge and never discovered the gauge invariance. I claim that they would never observe any contradiction between theory and experiment. If you agree with that statement (and I don't see any reason why shouldn't you), then it should be obvious they would have a Lorentz and gauge non-noninvariant theory that agrees with experiments.
What exactly does not make sense if you compute everything in a fixed gauge?vanhees71 said:If they discovered (classical or quantum) electrodynamics they'd also have discovered gauge invariance, because electrodynamics makes only mathematical sense as a gauge theory, let alone its success in describing all electromagnetic phenomena.
How is that relevant from a scientific point of view if that makes correct measurable predictions?vanhees71 said:Your (mis)interpretation of the Coulomb-gauge-fixed equations is a typical example. You claim there were actions at a distance, because you claim that the potentials were physical fields.