Encyclopedia Cosmology Cosmology Polarized Birth Domains Polarized Components Le Three
ARTICLE 2 claims 2 theorems
Cosmology Polarized Birth Domains Polarized Components Le Three
A theorem about a discrete grid shows a polarized birth field can always be carried by exactly three regions, regardless of the world's size.
The three-region bound
A ledger, a discrete record of events, can be organized in many ways. The question at hand is how many separate regions are needed to carry a particular kind of field, one that assigns a value of plus one to one half of a grid, minus one to the other half, and zero to the dividing line. The theorem polarized_components_le_three proves that this number is at most three, and in fact exactly three, for any radius of the grid in both two and three dimensions.
The proof works by defining a height function on the grid that decreases along edges connecting cells of the same charge. This height function has only three points where it reaches zero: one in the plus region, one in the minus region, and one on the spine. Since every cell descends along a monochromatic edge to one of these three roots, the entire grid is covered by at most three connected components. The theorem then shows the bound is sharp by exhibiting three cells of distinct charges that cannot be connected.
This result is significant because it establishes that the carried state of the birth field is sub-extensive: the number of regions does not grow with the volume of the world. A world of Θ(t^d) cells is carried by O(1) super-regions, so the fraction of components to volume tends to zero. This is the sharpest possible sub-extensivity, making the North-Star claim "carry each region at the coarsest φ-rung its recognition allows" exact for the birth configuration.
In Recognition Science, this theorem is part of a larger chain that forces the golden ratio, an eight-tick cycle, and three spatial dimensions from a single cost function. The polarization field is the configuration the shell creation installs each cadence cycle, so this bound describes the initial state of the universe in the framework's terms.
The theorem does not claim that the live engine maintains this bound. After birth, the spine diffuses by forced resolution, creating additional small interface components. Those are bounded above by a separate interface bound, not by this theorem. The statement is exact only for the forced conjugate birth configuration, not for the subsequent evolution.
THEOREM polarized_components_eq_three · polarized_components_eq_three · IndisputableMonolith/Cosmology/PolarizedBirthDomains.lean
/-- **The polarized birth field has exactly 3 locked domains, every radius (2-D).** The upper bound
`≤ 3` (descent toward the three roots) meets the lower bound `≥ 3` (the three roots carry the three
distinct charges `+1`, `-1`, `0`, and charge is a closure invariant). So the carried state is exactly
3 for all `t ≥ 1`: the fine half, the coarse half, and the spine. -/
theorem polarized_components_eq_three (t : ℕ) (ht : 1 ≤ t) : comp (Fmono t) = 3 := by
refine le_antisymm (polarized_components_le_three t ht) ?_
exact three_le_comp_of_three_charges (edges t) (polarized t)
⟨(1, 0), by rw [mem_ball_iff]; omega⟩
⟨(-1, 0), by rw [mem_ball_iff]; omega⟩
⟨(0, 0), by rw [mem_ball_iff]; omega⟩
(by simp only [polarized]; dsimp only; decide)
(by simp only [polarized]; dsimp only; decide)
(by simp only [polarized]; dsimp only; decide)
THEOREM polarized_carried_subextensive · polarized_carried_subextensive · IndisputableMonolith/Cosmology/PolarizedBirthDomains.lean
/-- **Carried-state sub-extensivity for the birth field (2-D).** The polarized diamond fills
`2t² + 2t + 1` cells (Phase 49) but is carried as exactly 3 super-regions, so the carried state times
the radius is at most the area for every `t ≥ 1`: `3 t ≤ card (ball t)`, the carried cost is `O(1)`
while the world is `Θ(t²)`. -/
theorem polarized_carried_subextensive (t : ℕ) (ht : 1 ≤ t) :
comp (Fmono t) = 3 ∧ 3 * t ≤ (InterfaceComponentBound.Diamond.ball t).card := by
refine ⟨polarized_components_eq_three t ht, ?_⟩
rw [LatticeBallVolume.Diamond.card_ball]
nlinarith [ht]
What this page does not claim
The theorem does not apply to the live engine's evolved state, only to the forced conjugate birth configuration. The theorem does not claim that the spine remains static; it diffuses after birth, creating additional components. The theorem does not establish the three-dimensionality of space; that is a separate result in the framework's forcing chain.
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expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
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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 interface bound for the live engine compare to the three-region bound for the birth field?
- What physical process corresponds to the diffusion of the spine after the birth configuration?
- Does the sub-extensivity result generalize to fields with more than three charge values?
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THEOREM polarized_components_eq_three · polarized_components_eq_three · IndisputableMonolith/Cosmology/PolarizedBirthDomains.lean
/-- **The polarized birth field has exactly 3 locked domains, every radius (2-D).** The upper bound `≤ 3` (descent toward the three roots) meets the lower bound `≥ 3` (the three roots carry the three distinct charges `+1`, `-1`, `0`, and charge is a closure invariant). So the carried state is exactly 3 for all `t ≥ 1`: the fine half, the coarse half, and the spine. -/ theorem polarized_components_eq_three (t : ℕ) (ht : 1 ≤ t) : comp (Fmono t) = 3 := by refine le_antisymm (polarized_components_le_three t ht) ?_ exact three_le_comp_of_three_charges (edges t) (polarized t) ⟨(1, 0), by rw [mem_ball_iff]; omega⟩ ⟨(-1, 0), by rw [mem_ball_iff]; omega⟩ ⟨(0, 0), by rw [mem_ball_iff]; omega⟩ (by simp only [polarized]; dsimp only; decide) (by simp only [polarized]; dsimp only; decide) (by simp only [polarized]; dsimp only; decide)The theorem polarized_components_le_three proves that this number is at most three, and in fact exactly three, for any radius of the grid in both two and three dimensions. polarized_components_eq_three · polarized_components_eq_three · IndisputableMonolith/Cosmology/PolarizedBirthDomains.leanTHEOREM polarized_carried_subextensive · polarized_carried_subextensive · IndisputableMonolith/Cosmology/PolarizedBirthDomains.lean
/-- **Carried-state sub-extensivity for the birth field (2-D).** The polarized diamond fills `2t² + 2t + 1` cells (Phase 49) but is carried as exactly 3 super-regions, so the carried state times the radius is at most the area for every `t ≥ 1`: `3 t ≤ card (ball t)`, the carried cost is `O(1)` while the world is `Θ(t²)`. -/ theorem polarized_carried_subextensive (t : ℕ) (ht : 1 ≤ t) : comp (Fmono t) = 3 ∧ 3 * t ≤ (InterfaceComponentBound.Diamond.ball t).card := by refine ⟨polarized_components_eq_three t ht, ?_⟩ rw [LatticeBallVolume.Diamond.card_ball] nlinarith [ht]A world of Θ(t^d) cells is carried by O(1) super-regions, so the fraction of components to volume tends to zero. polarized_carried_subextensive · polarized_carried_subextensive · IndisputableMonolith/Cosmology/PolarizedBirthDomains.lean