Can someone explain what's groundbreaking about this? Maybe it's not done so very rigorously, but pretty much every plasma physics textbook will contain a derivation of Boltzmann equation, including some form of collisional operator, starting from Liouville's theorem[1] and then derive a system of fluid equations [2] by computing the moments of Boltzmann equation.
John Baez wrote a Mastodon thread on this paper here:
https://mathstodon.xyz/@johncarlosbaez/114618637031193532
He references a posted comment by Shan Gao[^1] and writes that the problem still seems open, even if this is some good work.
[^1]: https://arxiv.org/abs/2504.06297
This is the larger part of the work:
https://arxiv.org/abs/2408.07818
Can someone explain what's groundbreaking about this? Maybe it's not done so very rigorously, but pretty much every plasma physics textbook will contain a derivation of Boltzmann equation, including some form of collisional operator, starting from Liouville's theorem[1] and then derive a system of fluid equations [2] by computing the moments of Boltzmann equation.
[1]: https://en.wikipedia.org/wiki/Liouville%27s_theorem_(Hamilto...
[2]: https://en.wikipedia.org/wiki/BBGKY_hierarchy
So where and how does a jump from nice symmetric reversible equations to turbulent irreversibility happen?
Sabine Hossenfelder's video on this: https://youtu.be/mxWJJl44UEQ
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