I'm still wondering about the physical interpretation of the action integral of some mechanical system (classical theory here, to simplify things): \begin{equation}\tag{1} A = \int_{t_1}^{t_2} L(q, \, \dot{q}) \, dt, \end{equation} where $L = K - U$ is the system's lagrangian. I'm not interested in its variation and the principle of extremal action. I'm interested in the number given by (1), wathever the motion (extremal or not). I was always amazed by some analogies with the statistical definition of entropy, defined on phase space ($k_B = 1$ here): \begin{equation}\tag{2} S = -\int_{\Omega} \rho \, \ln{\rho} \, d\Omega, \end{equation} especially when the probability density is Boltzmanian : $\rho \propto e^{-\, \beta H}$ (for equilibrium macroscopic states). The usual standard interpretation of entropy is this:
Entropy $S$ is a measure of the lack of the statistical knowledge that you need to define the microscopic state of a system at a given time.
I'm wondering about a similar (inverted) interpretation for the action (1) (this is my own interpretation):
Action $A$ is a measure of the mechanical information that you already have on the state of a system and its evolution during some time interval.
Is it possible to make that statement more precise and rigorous? Could we define (or give a sense to) mechanical information as the action integral, a bit like entropy as a measure of "ignorance" (average of $\sigma = -\, \ln{\rho}$)?
I've checked the similar questions on Stack Exchange, like this one : What is the significance of action?, but all of the answers are systematically refering to the extremal action principle (or stationary action principle), and they aren't answering the question about the action itself.
I don't think that the "action" is just an abstract tool (with a fancy mysterious name) to find the classical trajectories in phase space. And I don't think that Quantum Mechanics is giving any answer on the interpretation (action as a "phase variable", which is just pushing the question under the carpet).