It's true that the probability of a microstate is determined by energy and temperature, but the Maxwell-Boltzmann equation assumes that temperature is constant for all particles. Temperature is a distinguishing feature of two distributions, not of two particles within a distribution, and least-temperature is not a state that systems tend towards.
I know. Models are not particles. They are distributions over outcomes. They CAN be the trivial distributions over outcomes (X will happen).
I was not referring to either form of degenerate gas in any of my posts here, and I'm not sure why I would give that impression. I also did not use any conservation of information, though I can see why you would think I did, when I spoke of the information requirement. I meant simply that if you add 1 bit of information, you have added 1 bit of entropy - as opposed to in a physical system, where the Fermi shell at, say, 10 meV can have much more or less entropy than the Fermi shell at 5meV.
I thought you were referring to degenerate gases when you mentioned nontrivial behavior in solid state systems since that is the most obvious case where you get behavior that cannot be easily explained by the "obvious" model (the canonical ensemble). If you were thinking of something else, I'm curious to know what it was.
I'm having a hard time parsing your suggestion. The "dropout" method introduces entropy to "the model itself" (the conditional probabilities in the model), but it seems that's not what you're suggesting. You c...
A putative new idea for AI control; index here.
Noise versus preference and complexity
Error versus bias versus preference
Preference versus prejudice (and bias)
Known prejudices
Revisiting complexity