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@Demystifier , where do you see distinctions like Hamiltonian and variational methds, versus forces and Diff.. Eq. ?
The forum discussion centers on the distinction between theories and interpretations in quantum mechanics (QM), specifically addressing theories T1 (Heisenberg) and T2 (Schrödinger) as equivalent models. Participants argue that interpretations, such as the Copenhagen and Many-Worlds interpretations, do not constitute separate theories but rather different descriptions of the same underlying mathematical framework. The conversation highlights the limitations of discussing interpretations that yield the same experimental predictions, suggesting that such debates often lack resolution. The consensus leans towards merging the concepts of theory and model rather than theory and interpretation to clarify the discourse in quantum physics.
PREREQUISITESPhysicists, students of quantum mechanics, and researchers interested in the philosophical implications of theoretical models and interpretations in quantum physics.
They are not physical theories. They are mathematical tools that share some similarities but make fundamentally different statements.Auto-Didact said:How about
T1 Frequentist statistics
T2 Bayesian statistics
Yes, those could also be thought of as different theories with identical measurable predictions.PAllen said:@Demystifier , where do you see distinctions like Hamiltonian and variational methds, versus forces and Diff.. Eq. ?
For a non-quantum example see my post above. In your terminology, they would not be different theories too.martinbn said:I expected a non quantum example. So, you have in mind only QM interpretations, and you think they should be called theories. My opinion is that they are correctly called interpretations. The all start with QM or at least the core of QM, then add a bit more, yet don't get new predictions. To me that is not a different theory. To be a different theory it should build on something else, it should be possible to get to that theory even if you have never seen QM. And that is not the case of the interpretations.
fresh_42 said:a theory - or model - is a mathematical framework to describe the experimental results, including possible predictions. On the other hand, an interpretation is merely an informal description of named theory / model to describe the mathematical framework in common language and by the frequent use of aphorisms and metaphors.
Demystifier said:Some versions of BM do, but the standard "minimal" version doesn't.
BM is observationally equivalent to Copenhagen only in the FAPP sense.atyy said:But isn't one difference that the minimal version allows a measurement to be reversed in principle but not FAPP, whereas Copenhagen does not allow a measurement to be reversed in principle and FAPP since its principle is FAPP.
Also, is the equivalence of minimal BM and Copenhagen exact, or does minimal BM have small but FAPP unmeasurable differences from Copenhagen?
Thinking about the Wilson case, many expositions say that Wilsonian renormalization does produce terms different from old fashioned renormalization, but the differences are too small to be measured. So if one uses theory to mean exact equivalence, then Wilsonian renormalization is a different theory. However, since interpretation is also supposed to have the meaning of "solving a common sense problem with the theory (measurement for Copenhagen QM or nonsensical subtraction of infinities for old-fashioned renormalization", I would like to say Wilsonian renormalization is both an interpretation (solves the conceptual problem) and a different theory.
Demystifier said:BM is observationally equivalent to Copenhagen only in the FAPP sense.
Demystifier said:Can you give a reference for an exposition saying that Wilsonian renormalization produces terms different from old fashioned renormalization?
Brilliant insight atyy!atyy said:For that reason, I think even if one is not against "interpretation", minimal BM can be considered a different theory. In contrast, the Newtonian, Lagrangian, and Hamiltonian formulations would be identical even in principle so they are the same theory. Similarly, the Schroedinger and Heisenberg pictures are the same theory.
http://www.solvayinstitutes.be/pdf/doctoral/Adel_Bilal2014.pdf (p69)
Theories like QED are presently thought to be only effective theories ... Such an effective theory then has an effective Lagrangian obtained by “integrating out” the very heavy additional fields that are present in such theories. This necessarily results in the generation of (infinitely) many non-renormalizable interactions ... From the previous argument it is then clear that at energies well below this scale these additional non-renormalizable interactions are completely irrelevant, and this is why we only “see” the renormalizable interactions. Our “low-energy” world is described by renormalizable theories like QED not because such theories are somehow better behaved, but because these are the only relevant ones at low energies: Renormalizable interactions are those that are relevant at low energies, while non-renormalizable interactions are irrelevant at low energies.

Demystifier said:BM is observationally equivalent to Copenhagen only in the FAPP sense.
In principle, Bohmian particles may be far from the quantum equilibrium, in which case the probabilities of measurement outcomes can be totally different.PeterDonis said:What in principle predictions does BM make that are not equivalent to predictions of Copenhagen?
The term 'Copenhagen interpretation' suggests something more than just a spirit, such as some definite set of rules for interpreting the mathematical formalism of quantum mechanics, presumably dating back to the 1920s. However, no such text exists, apart from some informal popular lectures by Bohr and Heisenberg, which contradict each other on several important issues[citation needed]. It appears that the particular term, with its more definite sense, was coined by Heisenberg in the 1950s,[4] while criticizing alternate "interpretations" (e.g., David Bohm's[5]) that had been developed.[6] Lectures with the titles 'The Copenhagen Interpretation of Quantum Theory' and 'Criticisms and Counterproposals to the Copenhagen Interpretation', that Heisenberg delivered in 1955, are reprinted in the collection Physics and Philosophy.[7] Before the book was released for sale, Heisenberg privately expressed regret for having used the term, due to its suggestion of the existence of other interpretations, that he considered to be "nonsense".
https://en.wikipedia.org/wiki/Copenhagen_interpretation#Origin_of_the_term
If you want to take that road: Einstein, Schrödinger, Born and Dirac all spoke out against QM as being incomplete, tentative or in need of revision; moreover, Dirac also rightfully criticized QFT.bolbteppa said:the founders of QM, e.g.
In fact, Madelung published his equations (Nov 1926) a month before Schrödinger (Dec 1926). But arguing about priority is childish nonsense.bolbteppa said:such as dBB which steal equations from QM
Yeah, just like how Newton being 'obviously correct' for two centuries invalidated Einstein's attempt to rewrite the canon of physics... oh wait.bolbteppa said:The fact that one is led to do things like deny things like relativity as fundamental https://www.physicsforums.com/insights/stopped-worrying-learned-love-orthodox-quantum-mechanics/ and rationalize away such basic, basic, concepts of physics should prove to most people why words like "nonsense" for these alternatives are appropriate.
atyy said:Theories like QED are presently thought to be only effective theories
Do you mean the paper published in January 1926? “Quantisierung als Eigenwertproblem. Erste Mitteilung” (Quantization as a problem of proper values, part one), which he sent to the Annalen der Physik on 26 January 1926. In this paper, he first formulated his famous wave equation...” https://www.uzh.ch/en/about/portrait/nobelprize/schroedinger.htmlAuto-Didact said:(Snip) Schrödinger (Dec 1926) (snip).
He indeed derived it back in 1925 and published it quite early on. But as I said, arguing about priorities is childish especially seeing the extensive influencing the early founders had on each other (including Planck, Einstein, de Broglie et al.).*now* said:Do you mean the paper published in January 1926? “Quantisierung als Eigenwertproblem. Erste Mitteilung” (Quantization as a problem of proper values, part one), which he sent to the Annalen der Physik on 26 January 1926. In this paper, he first formulated his famous wave equation...” https://www.uzh.ch/en/about/portrait/nobelprize/schroedinger.html
bolbteppa said:and ironically in QM you can't derive the non-relativistic Schrödinger equation
Auto-Didact said:To get back on topic: orthodox QM has several problems; however, from both a pure mathematical point of view as well as the mathematical physics point of view, the most important problem is the ad hoc nature of the Born rule as an axiom
Auto-Didact said:than the disjointed mess that is orthodox QM.
bhobba said:Have you seen chapter 3 of Ballentine where its derived from probabilities are frame independent? If so can you elaborate on how it fits in with the above?
Thanks
Bill
bolbteppa said:My post said "without Galilean symmetry... you can't derive the non-relativistic Schrödinger equation BM'ers seem to think is all of reality", chapter 3 of Ballentine is mostly about applying Galilean symmetry in the edition I have seen anyway.
bhobba said:Yes - without something to be symmetrical in you can't apply symmetry. That's is the paradox about physics relation to symmetry despite is fundamental importance.
Thanks
Bill

bolbteppa said:The fact that one is led to do things like deny things like relativity as fundamental https://www.physicsforums.com/insights/stopped-worrying-learned-love-orthodox-quantum-mechanics/ and rationalize away such basic, basic, concepts of physics should prove to most people why words like "nonsense" for these alternatives are appropriate.
Demystifier said:In principle, Bohmian particles may be far from the quantum equilibrium, in which case the probabilities of measurement outcomes can be totally different.
It's a genuinely uncertain issue. There are known cases where adding an ##SU(2)## gauge field to otherwise trivial theories renders them non-trivial and there are numerical simulations and simplified or limiting theories suggesting this might be what occurs in the Electroweak theory. So we currently don't actually know if the standard model is trivial.bhobba said:Indeed. QED is even thought to be trivial, but I do not think anyone has proven it rigorously. If so that is strong evidence it could only be an effective theory - and of course we now know it is since its part of the electro-weak theory at high enough energies.
Is the elctro-weak theory trivial - that is something I have not seen anything written about - but my guess is probably.
Thanks
Bill
It is not my viewpoint, it is a standard one in mathematical physics, because historiclly almost all more fundamental mathematical reformulations were discovered from within this very viewpoint of practicing mathematical physics.bolbteppa said:The fact that you think we need to formulate theories in terms of differential equations is to unavoidably assume that classical paths must exist, and so to literally deny/misunderstand the most basic claim of QM that paths don't exist - if paths don't exist, all of classical physics is wrong and we have absolutely nothing...
##p=hk## is just another way of stating the de Broglie wavelength, which was invented in 1924 before Schrödinger came up with his equation. Again, it is irrelevant what happened first: the mathematical veracity of equations do not depend on when someone first writes them down or for whatever reasons they were written down.bolbteppa said:Please go and read Bohm's original papers (http://cqi.inf.usi.ch/qic/bohm1.pdf) and show me where he derived the Schrödinger equation - you won't find it because he didn't, he assumed it out of thin air, which is what many BM sources do. The ones that try harder try and derive it from something along the lines of these here https://en.wikipedia.org/wiki/De_Broglie–Bohm_theory#Derivations which are either complete nonsense (to be explained in a moment) or are using concepts that assume standard Copenhagen QM (I mean really, pμ=ℏkμpμ=ℏkμp^{\mu} = \hbar k^{\mu} as your starting point, where do these strange concepts of energy or momentum even come from? and we are talking about a theory that is not a 'disjointed mess') and so defeat the whole purpose of BM, i.e. to save classical physics and deny what science actually tells us...
Experiments say nothing of the sort, it is an interpretation of the theory and experiment together which talks about the non-existence of paths.bolbteppa said:All we can say before the Born rule is that paths don't exist because that's what experiments tell us, and therefore that classical theories (non-relativistic and relativistic) are wrong, and so we literally have nothing...
Again it's not my own viewpoint, it is a legitimate standard viewpoint in the practice of mathematical physics.bolbteppa said:The very fact you think we should be able to derive the Born rule illustrates an extremely fundamental misunderstanding of what QM says - if the very first thing it says is that path's don't exist, and so without paths we have nothing,
It is not shocking because all canonical physical theories, except for QM, were eventually able to be derived in such a manner, once reformulated into the specific mathematical framework in which the physical theory best fits (i.e. into vector calculus, or exterior calculus, or differential forms, or differential geometry, or bispinor calculus, or complex manifolds, etc) by the mathematicians and mathematical physicists.bolbteppa said:the idea we need to derive the premise on which the whole theory is built is simply shocking,
The principle of least action is directly derivable from Stokes theorem; calculus of variations is not an independent framework but a direct consequence of not taking exterior calculus and differential forms to heart.bolbteppa said:if properly understood it's like saying we need to derive F = ma or the principle of least action from nothing...
This is just one way of seeing it, i.e. an interpretation. It is however not merely an interpretation of an equation but an interpretation of methodology as well; i.e. it is a purely pragmatic FAPP philosophy. In terms of mathematical physics, such FAPP philosophies are unnecessary assumptions since the question to be answered in mathematical physics isn't a question to be answered FAPP, but instead a question to be answered in principle.bolbteppa said:In order to state something to build a theory we need to admit that we have the existence of classical mechanics in 'some sense', i.e. the to-be-defined quasi-classical limit, and so try to merge the fact that paths don't exist in experiments with paths existing in some approximate sense which leads to needing what we call the Born rule, which is why QM is so nuts - we unavoidably need classical mechanics to formulate it.
This is just pure hogwash. Wave functions are just mathematical objects, taken literally functions describing waves. They arise naturally not only in physics, but in all different kinds of manners in empirical and phenomenological science studied by applied mathematicians and/or non-physicist scientists.bolbteppa said:Without standard QM you are literally banned from using concepts like wave functions as if they were fundamental, it is simply madness to even think of something like a wave function if the notion of a path exists in any sense, nothing but a decision to ignore inherently obtainable information for no reason,
The theory of differential equations absolutely says no such thing; what can and cannot be done depends on the class of the differential equation. It is a severe misapprehension of mathematics to think otherwise. It is not a non-trivial issue because the theory of differential equations is still a work in progress, meaning many physicists, focussed solely on applications, remain unaware of such issues.bolbteppa said:and the ironic reason for this is differential equations, which tell us that if particles follow any kind of path at all in any sense, we should be able to predict the path no matter what the equations which control it's motion are because it's just basic mathematics
Again what I stated applies to all of canonical physics, up to and including statistical mechanics, critical phenomenon, geometrodynamics, etc.bolbteppa said:just because Newton and Einstein got the force laws (i.e. part of the ode's) allowing us to predict the motion wrong
Opinion, not fact. Whether this opinion is popular among physicists says absolutely nothing about the veracity of the claim.bolbteppa said:if the paths exist in any sense, you'd have to deny differential equations if you want to pretend we can never know what the path was for some given special example, which is why said 'derivations' of the Schrödinger equation are complete nonsense
The reasons Bohr et al. made such strong claims were due to reasons of practicality and ignorance of more advanced mathematics; they were at the cutting edge in their time. Realizing that much more was left to be understood experimentally, physicists generally just ignored the problem in the foundations of QM for almost a century, merely pretending that these were resolved, which is why the foundational problems still haunts the theory until this very day.bolbteppa said:the idea that these random concepts like wave functions should mean anything if paths exist is simply human bias, of course it's a bias motivated by BM'ers trying to copy orthodox QM because they have to for unexplained reasons despite the fact that they should be able to do way more fundamental things like actually predict paths if what they claimed made any sense... In other words, there are good reasons why the founders made such bold claims about complementarity e.g. paths not existing and why this is all they could come up with without committing basic logical errors...
Easy, two different ways:bolbteppa said:Landau's QM spends a good few pages stressing the technical points here, I don't know how anybody could try and imply that orthodox QM is flawed because the Born rule can't be found via differential equations if they understood the very first claim of QM is that paths simply don't exist so that no differential equation could ever dictate it's most fundamental claim...
That depends on the intent of the formulation. The intent in mathematical physics is to give QM a solid mathematical foundation instead of parroting FAPP philosophy; no one seems to question the non-FAPP intent of mathematical physics when Wightman et al. attempted to give a rigorous foundation of QFT. I'm guessing you would say that Newton-Cartan theory has absolutely no scientific merit either and studying it was a complete waste of time for physicists.bolbteppa said:Even more laughable is the idea that a quantum theory which fails so spectacularly at dealing with relativity is "a fundamentally more coherent mathematical framework than the disjointed mess that is orthodox QM",
That is a way, not the only way. And yes, it is still mathematically more coherent independent of whether it is the correct theory of nature. That is another question entirely! Fact: BM as well as Newton-Cartan theory are more coherent mathematical frameworks than orthodox QM. This just implies that mathematical coherence alone is not sufficient nor the best guide for judging the utility or veracity of a theory for physics; this is obvious, that role belongs to experiment.bolbteppa said:as I've already pointed out one of the ways people claim to be able to do this is to literally deny that special/general relativity is more fundamental non-relativistic classical mechanics, this should be beyond shocking, yet in here we are implying this is "more coherent"?
Without symplectic geometry there is no principle of stationary anything. Working on BM as a project in terms of mathematical physics does not in any way imply that those who work on it believe it to be all of reality; that is just pure projection, which in fact sounds very much like a soundbite that a politician would make to smear his opponents.bolbteppa said:Finally, the reason physicists are "ranting on about the fundamental importance of symmetries" is because without symmetries we can do almost nothing, e.g. without Galilean symmetry we can't go far beyond the statement of the principle of Least action in non-relativistic mechanics, and ironically in QM you can't derive the non-relativistic Schrödinger equation BM'ers seem to think is all of reality, and it's merely the failure of Galilean symmetry that leads to special relativity, with both Galilean and Einsteinian relativity based on the primitive notion of a path existing, unlike QM... (Again, all in Landau).
I see no issue whatsoever with constructing intermediate mathematical frameworks in order to arrive at a new physical theory or in trying to formulate rigorous foundations where they are sorely lacking in an existing physical theory. The progression in the foundations of physics is not helped at all by physicists who believe that appealing to FAPP philosophy actually solves foundational problems, thereby giving them a license to bark at those actually attempting to solve such foundational problems.bolbteppa said:So yes, BM is "actually practically a different theory from orthodox QM" because it begins by contradicting the most basic claim QM makes and then tries to still get the results of the theory it denies by assuming it's equations out of thin air, it's no wonder people like Heisenberg used words like "nonsense" for alternatives this logically flawed, with the relativity denial issues taking this over the top. These are the kinds of serious flaws that an essay like this is trying to legitimize...
I certainly agree with that.atyy said:Thus if QM is not the same theory as QM, then BM is not the same theory as QM.
Yes, the first communication article instead seems to be the article in question. Responding to a request in another thread here I’d linked a paper recently that discusses the first two of a number of his articles published in 1926, including the first communication article, hence some interest in the facts. The paper I recently linked also describes aspects of notions involved in the wave equation as misleading, hence less interest in primacies here : https://royalsocietypublishing.org/doi/pdf/10.1098/rsta.2017.0312.Auto-Didact said:He indeed derived it back in 1925 and published it quite early on.