Encyclopedia Foundation Foundation Ground State Dynamics
ARTICLE 3 claims 3 theorems
Foundation Ground State Dynamics
In Recognition Science, a system at rest must sit at the lowest point of its own conserved sector, and in a neutral sector that point is always the all-ones configuration.
The stable ground state
Foundation ground state dynamics is the study of what a recognition system does when nothing pushes on it. The framework models a system as a ledger, a discrete record of events, whose state is a configuration of positive numbers, one per channel. Dynamics enters through a variational rule: the next state is chosen to lower a conserved quantity, much as a ball rolls downhill until it reaches a valley floor. The first theorem of the module states that any equilibrium, any state that persists unchanged, coincides exactly with the uniform minimizer of its conserved sector. In plain words, a system at rest has no choice but to sit at the lowest point of its own configuration space.
The second theorem sharpens this for a special sector. Each configuration carries a quantity called its log-charge, a measure of how far its entries sit from unity on a logarithmic scale. When that charge is zero, the sector is neutral, and the unique equilibrium is the unity configuration, the state where every channel holds the number 1. The proof is short and direct: the equilibrium must equal the uniform minimizer, and in a zero-charge sector the uniform minimizer is exactly the all-ones state. This is not a numerical coincidence; it is a forced equality, derived from the variational rule and the definition of charge.
The module then packages this result for the simplest possible system, a single channel holding one ratio r. A one-channel ratio is just a positive real number, and its log-charge is the ordinary natural logarithm of r. In the neutral sector, where log r equals zero, the stability condition forces r to equal 1. The theorem stable_zero_charge_ratio_eq_one states this cleanly: a stable one-channel ratio in the neutral sector is unity. This is the dynamic counterpart of the static cost result; where the cost function forces the golden ratio as the unique self-similar scaling, the dynamic rule forces the neutral ground state to be the identity.
What this changes is the picture of what "rest" means in the framework. Rest is not a default or a choice; it is a consequence of the variational rule, and in a neutral sector it is unique. The all-ones configuration is not merely a convenient baseline; it is the only state that survives the requirement of stability. This gives the framework a concrete anchor point: when a system carries no net charge, its ground state is the unity configuration, and any deviation from unity requires a nonzero charge to sustain it.
THEOREM equilibrium_entries_eq_uniform · IndisputableMonolith/Foundation/GroundStateDynamics.lean
/-- Any equilibrium coincides with the uniform minimizer of its conserved sector. -/
theorem equilibrium_entries_eq_uniform {N : ℕ} (hN : 0 < N)
(c : Configuration N) (hEq : IsEquilibrium c) :
c.entries = (uniform_config hN (log_charge c)).entries := by
exact variational_step_unique hN c c (uniform_config hN (log_charge c))
hEq (uniform_is_variational_successor hN c)
THEOREM zero_charge_equilibrium_is_unity · IndisputableMonolith/Foundation/GroundStateDynamics.lean
/-- The zero-charge equilibrium is the unity configuration. -/
theorem zero_charge_equilibrium_is_unity {N : ℕ} (hN : 0 < N)
(c : Configuration N) (hEq : IsEquilibrium c)
(hCharge : log_charge c = 0) :
c.entries = (unity_config N hN).entries := by
calc
c.entries = (uniform_config hN (log_charge c)).entries :=
equilibrium_entries_eq_uniform hN c hEq
_ = (uniform_config hN 0).entries := by rw [hCharge]
_ = (unity_config N hN).entries := by
funext i
simp [uniform_config, unity_config]
THEOREM stable_zero_charge_ratio_eq_one · IndisputableMonolith/Foundation/GroundStateDynamics.lean
/-- Stable one-channel ratios in the neutral sector are forced to unity. -/
theorem stable_zero_charge_ratio_eq_one (r : ℝ) (hr : 0 < r)
(hEq : IsEquilibrium (ratioConfig r hr))
(hCharge : log_charge (ratioConfig r hr) = 0) :
r = 1 := by
have hEntries :
(ratioConfig r hr).entries = (unity_config 1 (by norm_num)).entries :=
zero_charge_equilibrium_is_unity (N := 1) (by norm_num) (ratioConfig r hr) hEq hCharge
have h0 := congrFun hEntries ⟨0, by simp⟩
simpa [ratioConfig, unity_config] using h0
What this page does not claim
The module does not derive the value of the golden ratio or any other constant. The module does not claim that all physical systems reach their equilibrium. The module does not address what happens outside the zero-charge sector.
Verify this page
Every tagged claim above names its theorem. To check one yourself rather than trust this page, elaborate the source module with Lean 4 and audit its axiom basis:
$ lake env lean IndisputableMonolith/Foundation/GroundStateDynamics.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
A page whose claims cannot be reproduced this way does not ship. In production, every anchor links to the exact declaration in the public source release, and this block carries the build receipt for the page itself.
Derived articles
This page is generated by a question-recursion engine: the questions its answers raise become the next pages. The current agenda, with open targets marked red:
- How does the variational rule connect to the cost function J that forces the golden ratio?
- What physical systems does the framework identify as zero-charge sectors?
- How does the unity ground state relate to the eight-tick recognition cycle?
- What happens to the ground state when the log-charge is nonzero?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM equilibrium_entries_eq_uniform · IndisputableMonolith/Foundation/GroundStateDynamics.lean
/-- Any equilibrium coincides with the uniform minimizer of its conserved sector. -/ theorem equilibrium_entries_eq_uniform {N : ℕ} (hN : 0 < N) (c : Configuration N) (hEq : IsEquilibrium c) : c.entries = (uniform_config hN (log_charge c)).entries := by exact variational_step_unique hN c c (uniform_config hN (log_charge c)) hEq (uniform_is_variational_successor hN c)Any equilibrium coincides with the uniform minimizer of its conserved sector. equilibrium_entries_eq_uniform · IndisputableMonolith/Foundation/GroundStateDynamics.leanTHEOREM zero_charge_equilibrium_is_unity · IndisputableMonolith/Foundation/GroundStateDynamics.lean
/-- The zero-charge equilibrium is the unity configuration. -/ theorem zero_charge_equilibrium_is_unity {N : ℕ} (hN : 0 < N) (c : Configuration N) (hEq : IsEquilibrium c) (hCharge : log_charge c = 0) : c.entries = (unity_config N hN).entries := by calc c.entries = (uniform_config hN (log_charge c)).entries := equilibrium_entries_eq_uniform hN c hEq _ = (uniform_config hN 0).entries := by rw [hCharge] _ = (unity_config N hN).entries := by funext i simp [uniform_config, unity_config]The zero-charge equilibrium is the unity configuration. zero_charge_equilibrium_is_unity · IndisputableMonolith/Foundation/GroundStateDynamics.leanTHEOREM stable_zero_charge_ratio_eq_one · IndisputableMonolith/Foundation/GroundStateDynamics.lean
/-- Stable one-channel ratios in the neutral sector are forced to unity. -/ theorem stable_zero_charge_ratio_eq_one (r : ℝ) (hr : 0 < r) (hEq : IsEquilibrium (ratioConfig r hr)) (hCharge : log_charge (ratioConfig r hr) = 0) : r = 1 := by have hEntries : (ratioConfig r hr).entries = (unity_config 1 (by norm_num)).entries := zero_charge_equilibrium_is_unity (N := 1) (by norm_num) (ratioConfig r hr) hEq hCharge have h0 := congrFun hEntries ⟨0, by simp⟩ simpa [ratioConfig, unity_config] using h0Stable one-channel ratios in the neutral sector are forced to unity. stable_zero_charge_ratio_eq_one · IndisputableMonolith/Foundation/GroundStateDynamics.lean