Peter Morgan
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No-one responded to this comment on Facebook (https://www.facebook.com/groups/2204629320/permalink/10156235771439321/?comment_id=10156240941494321), so I'll make it here also and make a few additional comments to reflect the discussion above, "Not only is classical physics not wrong, it is more capable than generally understood. If we present classical mechanics as a commutative algebra of operators together with a noncommutative algebra of transformations constructed using the Poisson bracket, all acting on a Hilbert space in a Koopman-von Neumann formalism, a random field CM can even be equivalent to a QFT if there is a natural complex structure (which there is in the case of electromagnetism, provided by the Hodge dual)."
This obviously leads in a slightly different direction than either ZapperZ's article or the comments above. Seeing one concern expressed in the comments above, I'll also note that I take not only the Lagrangian and Hamiltonian formalisms to be part of "Newtonian physics", but also Liouvillean probability densities over phase space and the Koopman-von Neumann formalism, and the extensions into issues of analysis (random fields, say, citing my own preference because they they can be made to parallel quantum fields so closely, but there are other stochastic approaches) that are required to discuss probability densities in field theory cases.
A further comment, about special relativity: the wave equation, the Klein-Gordon equation, and any differential equation that is Lorentz invariant, fit into the Lagrangian, Hamiltonian, Liouvillean, and Koopman-von Neumann formalisms well enough, so there's not any necessity to consider a limit as the speed of light is much larger than characteristic velocities. Just solve the equations.
I should be open about this comment being part of an effort to get more good mathematical physicists to look at and send me comments on https://arxiv.org/abs/1709.06711. The math there has been stable for many months, but the abstract and introduction do not discuss the relationship between random fields and quantum fields as clearly as I would like (nor as clearly as those people who have looked at the paper would like). I am now very close to submitting to a journal, so if you decide to have a look please be quick! I will be happy to send a copy of the paper as I currently have it to anyone who expresses interest.
This obviously leads in a slightly different direction than either ZapperZ's article or the comments above. Seeing one concern expressed in the comments above, I'll also note that I take not only the Lagrangian and Hamiltonian formalisms to be part of "Newtonian physics", but also Liouvillean probability densities over phase space and the Koopman-von Neumann formalism, and the extensions into issues of analysis (random fields, say, citing my own preference because they they can be made to parallel quantum fields so closely, but there are other stochastic approaches) that are required to discuss probability densities in field theory cases.
A further comment, about special relativity: the wave equation, the Klein-Gordon equation, and any differential equation that is Lorentz invariant, fit into the Lagrangian, Hamiltonian, Liouvillean, and Koopman-von Neumann formalisms well enough, so there's not any necessity to consider a limit as the speed of light is much larger than characteristic velocities. Just solve the equations.
I should be open about this comment being part of an effort to get more good mathematical physicists to look at and send me comments on https://arxiv.org/abs/1709.06711. The math there has been stable for many months, but the abstract and introduction do not discuss the relationship between random fields and quantum fields as clearly as I would like (nor as clearly as those people who have looked at the paper would like). I am now very close to submitting to a journal, so if you decide to have a look please be quick! I will be happy to send a copy of the paper as I currently have it to anyone who expresses interest.