iste said:
I might try to find exactly where in videos but pretty sure Barandes talks about the towers of probabilities for a stochastic process and that we don't have epistemic access to them and Albert I think tries to get Barandes to say they are not specified by the theory.
gentzen said:
In the end, he might land a bit too close to Fra/Fredrik, because he doesn't necessarily get laws of physics from his approach, and is actually happy with that.
Morbert said:
What I was hoping for was these towers of probabilities giving rise to inaccessible probabilities for trajectories that are nevertheless regular or lawlike. I fully accept that there are in principle probabilities for trajectories.
iste said:
On that same video there are statements of the sort all through about 1:17 to 1:46, and quite a clear concise summary from about 1:42 - 1:46. Barandes says these trajecyory probabilities exist but we have no epistemic access to them.
iste said:
Well, they could be lawlike, Barandes isn't specifying whether they are lawlike or not because he doesn't have any access to them.
Would you agree that these are the same probabilities he talks about in 2.2 In his
correspondence paper where he says
"In particular, probabilities assigned to whole trajectories, as constructed from higher-order conditional probabilities in the sense of (10), are then left unspecified as well."
I now listened to the key part where Albert keeps asking what is the fundamental law but isn't satisfied with Barandes saying "it's just stochastic", while Barandes struggles with understanding the category of answer Albert wants, which seem to reason from the traditional equation/system paradigm with initial/boundary conditions. As Barandes points out, the "law" is probably not best cast that way. But Albert don't seem convinced.
I see how the reaons is not convincing from Barandes presentation alone; to someone with a deep stance in the traditional paradigm. I follow Barandes logic, but its because I am already roughly on the same page to start with, I didn't need to be convinced. And my own arguments would necessarily go beyond the discussion and likely cause more confusion.
** In QM standard hilbert picture.This is system dynamics, and DYNAMICAL law encoded in the hamiltonian (or alternatively the equations of motion)
** In stochastic picture.There exists no traditional dynamical law. "Time evolution" is just a stochastic process in configuration space. No time evolution law is needed. But the process is constrained by Gamma,
Although different, I think gamma loosely encode what the hamiltonian encode.
So instead of asking why this hamiltonian, how to understand the internal structure of the hamiltonian, Barandes says its "just a stochastic processs", there is no fundamental "dynamical law". There is no NEED for more. But instead we need to ask, why the particular stochastic constraint Gamma; and what the particular configuration space. No of that is innocent. I think Barandes does not speak much about this because the same "fine tuning" exists i hilbert picture. So this is not a NEW problem, and its not the problem his correspondence is set out to solve, at least not at this stage.
For ME this is a key point, and i think conceptually contemplating emergent gamma is easier than emergent hamiltonian (although it is a different discussion) But I think Albert's objection is simply that he feels there must still be a dynamical law behind a stochastic model (just like there is in statistical mechanics). This is perhaps why he says to Barandes "you cant just say its a stochastic system". But I would say that to really appreciate the stochastic picture, a paradigm shift of thinking about physical theory is needed, as it boils down to the question, exactly WHY is the stochastic picutre better? And what is the difference to the simlpe statistical mechanics and entropic dynamics?
About the higher order probabilities, that one CAN contemplate for general stochastic processes (but that aren't needed in Barandes picture), are IMHO not relevant for normative probabilities. They makes no sense from my perspective at least (as normative in an agent picture), the history should be implicit in Gamma itself. I think the first order transitiions are sufficient, because they answer what i think is the only relevant question. P(future|now) - but, there is more information in here than the state of NOW, in the general case I think P itself evolves. But this is not true for a "stable quantum system". So this discussion gets us to the fringe of things.
Because the previous state history would refer to the systems own path, and from inference perspective, it is intutitive to me that these have no role to play because the system should have learn what cna be learned from its own histroy, or something is wrong. They may be allowed, but I see them as serving no purpose. This is just my hunch about this. I'm guessing there is a reason why Barandes leaves this murky stuff for future work. As it in itself, has no role to play for the stochastic quantum correspondnece as i see it.
/Fredrik