Discard spacetime distances but retain a Fisher geometry on probability distributions over events/causal relations. If “I” is written upstairs as a continuum MFI functional,
Discard spacetime distances but retain a Fisher geometry on probability distributions over events/causal relations. If “I” is written upstairs as a continuum MFI functional,
Define links (adjacency) without metric data by the cover relation: eᵢ ≺· eⱼ ⇔ (eᵢ ≺ eⱼ) and there is no eₖ such that eᵢ ≺ eₖ ≺ eⱼ. ST metric discarded, info geo can remain
Define links (adjacency) without metric data by the cover relation: eᵢ ≺· eⱼ ⇔ (eᵢ ≺ eⱼ) and there is no eₖ such that eᵢ ≺ eₖ ≺ eⱼ. ST metric discarded, info geo can remain
Random Insight: Today's Laplace's Demon is basically Simulation Theory (or religion), but there were a lot less claims of Laplace's Demon being real. Don't need either for determinism.
Random Insight: Today's Laplace's Demon is basically Simulation Theory (or religion), but there were a lot less claims of Laplace's Demon being real. Don't need either for determinism.
Same L-B: Q=−(ħ^2/2)(Δ_G R)/R + α ℛ(G).
Directional response without Fisher still has Distinguishability: R sets the relational metric tensor; its curvature guides motion.
Θ→0: conformal CJ; push-forward via K ⇒ EH
Same L-B: Q=−(ħ^2/2)(Δ_G R)/R + α ℛ(G).
Directional response without Fisher still has Distinguishability: R sets the relational metric tensor; its curvature guides motion.
Θ→0: conformal CJ; push-forward via K ⇒ EH