Encyclopedia Masses Masses Mass Genesis T10 Hypercube Substrate Substrate Graph Forced By Atomicity
ARTICLE 4 claims 4 theorems
Masses Mass Genesis T10 Hypercube Substrate Substrate Graph Forced By Atomicity
A machine-checked library proves that the ledger of recognition events forces a hypercube graph, and it does not predict which masses exist.
The substrate graph
A hypercube is a graph built from binary strings: each vertex is a sequence of bits, and two vertices are connected when their strings differ in exactly one position. A 3-dimensional hypercube is a cube, with 8 vertices and 12 edges. The framework's machine-checked library of formal theorems proves that the graph of legal recognition events, called the substrate graph, must be a hypercube. The proof starts from ledger atomicity, the rule that each recognition event changes exactly one bit of a pattern, and derives the graph structure rather than assuming it.
The library proves the edge count: a d-dimensional hypercube has d times 2 to the power (d minus 1) undirected edges. It proves that a single vertex has d edges leaving it, and that the largest possible cut, the number of edges crossing a division of vertices into two groups, equals that same total. These are theorems about the hypercube, checked by the machine, with no gaps and no extra axioms beyond the standard logical ones.
In Recognition Science, the framework models particle masses as arising from a ledger, a discrete record of recognition events. The graph result is a structural fact about that ledger. The framework proves the graph is a hypercube, but it does not derive the dimension d. The dimension is left open; the library only proves that if the measured lepton ratios are supported, then d must be at least 13 for the tau and at least 9 for the muon. These are lower bounds from measured values, not predictions of a specific dimension.
The wall, the maximum number of edges crossing a division of the hypercube, is an upper bound on what the substrate can support. It does not say which masses exist. The mass-genesis modules use d equals 3, giving a wall of 12, but whether dimensions above 3 are legitimate in this framework remains an open target. The theorem establishes the graph shape; it does not establish the physics of which masses appear.
What the result changes is the starting point for mass theory: the substrate is not a free choice but a forced structure. A reader can now see that the hypercube is not an assumption but a consequence of atomicity. The open question is which dimension is real, and that question is not settled by this declaration.
THEOREM t10HypercubeSubstrateCert · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
theorem t10HypercubeSubstrateCert : T10HypercubeSubstrateCert where
oneBitDiff_iff_adj := oneBitDiff_iff_hypercubeAdj
legal_tick_is_hypercube_edge := legalAtomicTick_hypercubeAdj
post_realizes_flip := post_hypercubeAdj
bipartite := hypercubeAdj_hammingWeight_parity
xor_preserves_adj := xorBy_hypercubeAdj
xor_transitive := xorBy_transitive
evenClass_attains_maxcut := fun _ hd => hypercubeCut_evenClass hd
singleton_cut_eq_degree := hypercubeCut_singleton
connectivity_three := hypercubeEdgeConnectivity_three
wall_three := hypercube_wall_three_ratio
muon_forces_d := fun _ h => muon_ratio_forces_accounts h
tau_forces_d := fun _ h => tau_ratio_forces_accounts h
muon_forces_cells := fun _ h => muon_ratio_forces_three_cells h
tau_forces_cells := fun _ h => tau_ratio_forces_five_cells h
posting_witness := posting_realizes_named_hypercube_edge
scope_does_not_derive_d := trivial
scope_wall_is_capacity_not_prediction := trivial
scope_d_gt_three_is_open := trivial
THEOREM card_directedHypercubeEdges · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
lemma card_directedHypercubeEdges (d : Nat) :
(directedHypercubeEdges d).card = d * 2 ^ d := by
classical
have hpart :
(directedHypercubeEdges d).card =
∑ p : Pattern d,
((directedHypercubeEdges d).filter (fun e => e.1 = p)).card := by
simpa [directedHypercubeEdges] using
(Finset.card_eq_sum_card_fiberwise
(s := directedHypercubeEdges d) (f := Prod.fst) (t := Finset.univ)
(fun _ _ => Finset.mem_univ _))
refine hpart.trans ?_
have hfiber (p : Pattern d) :
((directedHypercubeEdges d).filter (fun e => e.1 = p)).card = d := by
let N := Finset.univ.filter (fun q : Pattern d => HypercubeAdj p q)
have hset :
(directedHypercubeEdges d).filter (fun e => e.1 = p) =
N.image (fun q => (p, q)) := by
ext e
constructor
· intro he
rcases Finset.mem_filter.mp he with ⟨he', hp⟩
rcases Finset.mem_filter.mp he' with ⟨_, hadj⟩
exact Finset.mem_image.mpr
⟨e.2, by simp [N, hp ▸ hadj], Prod.ext hp.symm rfl⟩
· intro he
rcases Finset.mem_image.mp he with ⟨q, hq, rfl⟩
simp only [Finset.mem_filter, Finset.mem_univ, true_and, N] at hq
exact Finset.mem_filter.mpr
⟨Finset.mem_filter.mpr ⟨Finset.mem_univ _, hq⟩, rfl⟩
have hinj : Set.InjOn (fun q : Pattern d => (p, q)) N := by
intro _ _ _ _ h; exact (Prod.mk.inj h).2
rw [hset, Finset.card_image_of_injOn hinj, card_neighbors]
simp_rw [hfiber]
simp [Finset.sum_const, Patterns.card_pattern, Nat.mul_comm]
THEOREM hypercubeCut_le_total · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
/-- H5 ceiling. -/
theorem hypercubeCut_le_total {d : Nat} (A : Finset (Pattern d)) :
hypercubeCut A ≤ d * 2 ^ (d - 1) := by
classical
cases d with
| zero =>
have hz : hypercubeCut A = 0 := by
unfold hypercubeCut
refine Finset.card_eq_zero.mpr ?_
ext e
simp only [Finset.notMem_empty, iff_false, Finset.mem_filter,
Finset.mem_univ, true_and, HypercubeAdj]
intro h
-- no edges when there are no coordinates
have : (Finset.univ : Finset (Fin 0)).card = 0 := by simp
have hle := Finset.card_filter_le
(s := (Finset.univ : Finset (Fin 0)))
(p := fun i => e.1 i ≠ e.2 i)
omega
simp [hz]
| succ d' =>
have hdir := card_directedHypercubeEdges (d' + 1)
-- cut A ≤ half of directed edges via cut A = cut Aᶜ
let Cut := Finset.univ.filter fun e : Pattern (d'+1) × Pattern (d'+1) =>
HypercubeAdj e.1 e.2 ∧ e.1 ∈ A ∧ e.2 ∉ A
let Cut' := Finset.univ.filter fun e : Pattern (d'+1) × Pattern (d'+1) =>
HypercubeAdj e.1 e.2 ∧ e.1 ∉ A ∧ e.2 ∈ A
let swapE := fun e : Pattern (d'+1) × Pattern (d'+1) => (e.2, e.1)
have himage : Cut.image swapE = Cut' := by
ext e
constructor
· intro he
rcases Finset.mem_image.mp he with ⟨e', he', rfl⟩
rcases Finset.mem_filter.mp he' with ⟨_, hadj, hA, hnA⟩
exact Finset.mem_filter.mpr ⟨Finset.mem_univ _, hypercubeAdj_symm hadj, hnA, hA⟩
· intro he
rcases Finset.mem_filter.mp he with ⟨_, hadj, hnA, hA⟩
exact Finset.mem_image.mpr
⟨(e.2, e.1),
Finset.mem_filter.mpr ⟨Finset.mem_univ _, hypercubeAdj_symm hadj, hA, hnA⟩, rfl⟩
have hinj : Set.InjOn swapE Cut := by
intro x _ y _ h; exact Prod.ext (Prod.mk.inj h).2 (Prod.mk.inj h).1
have hcuts : Cut.card = Cut'.card := by
have := congrArg Finset.card himage
rwa [Finset.card_image_of_injOn hinj] at this
have hdisj : Disjoint Cut Cut' := by
refine Finset.disjoint_left.mpr ?_
intro e he1 he2
exact (Finset.mem_filter.mp he2).2.2.1 (Finset.mem_filter.mp he1).2.2.1
have hsub : Cut ∪ Cut' ⊆ directedHypercubeEdges (d'+1) := by
intro e he
simp only [Finset.mem_union, Cut, Cut', Finset.mem_filter,
directedHypercubeEdges] at he ⊢
rcases he with ⟨_, hadj, _, _⟩ | ⟨_, hadj, _, _⟩ <;>
exact ⟨Finset.mem_univ _, hadj⟩
have hle : 2 * Cut.card ≤ (directedHypercubeEdges (d'+1)).card := by
have := Finset.card_le_card hsub
have hu := Finset.card_union_of_disjoint hdisj
have : Cut.card + Cut'.card ≤ (directedHypercubeEdges (d'+1)).card := by
simpa [hu] using this
simpa [two_mul, hcuts] using this
have : Cut.card ≤ (d'+1) * 2 ^ d' := by
have h2 : 2 * Cut.card ≤ (d'+1) * 2 ^ (d'+1) := by simpa [hdir] using hle
have hpow : (d'+1) * 2 ^ (d'+1) = 2 * ((d'+1) * 2 ^ d') := by
rw [pow_succ]; ring
have h2' : 2 * Cut.card ≤ 2 * ((d'+1) * 2 ^ d') := by simpa [hpow] using h2
exact Nat.le_of_mul_le_mul_left h2' (by decide : 0 < 2)
simpa [hypercubeCut, Cut] using this
THEOREM tau_ratio_forces_accounts · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
theorem tau_ratio_forces_accounts {d : Nat}
(h : (347723 : ℚ) / 100 ≤ (2 : ℚ) ^ (d - 1)) : 13 ≤ d := by
by_contra hlt; push_neg at hlt; interval_cases d <;> norm_num at h
What this page does not claim
The declaration does not claim that any particular mass exists. The declaration does not claim that d equals 3 is the physically correct dimension. The declaration does not claim that the substrate graph is the only structure in mass genesis.
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/Masses/MassGenesis/T10HypercubeSubstrate.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:
- What physical principle, if any, selects the dimension d of the substrate graph?
- How does the hypercube graph connect to the measured masses of the charged leptons?
- What does it mean for a substrate to support a mass ratio, and what are the limits of that support?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM t10HypercubeSubstrateCert · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
theorem t10HypercubeSubstrateCert : T10HypercubeSubstrateCert where oneBitDiff_iff_adj := oneBitDiff_iff_hypercubeAdj legal_tick_is_hypercube_edge := legalAtomicTick_hypercubeAdj post_realizes_flip := post_hypercubeAdj bipartite := hypercubeAdj_hammingWeight_parity xor_preserves_adj := xorBy_hypercubeAdj xor_transitive := xorBy_transitive evenClass_attains_maxcut := fun _ hd => hypercubeCut_evenClass hd singleton_cut_eq_degree := hypercubeCut_singleton connectivity_three := hypercubeEdgeConnectivity_three wall_three := hypercube_wall_three_ratio muon_forces_d := fun _ h => muon_ratio_forces_accounts h tau_forces_d := fun _ h => tau_ratio_forces_accounts h muon_forces_cells := fun _ h => muon_ratio_forces_three_cells h tau_forces_cells := fun _ h => tau_ratio_forces_five_cells h posting_witness := posting_realizes_named_hypercube_edge scope_does_not_derive_d := trivial scope_wall_is_capacity_not_prediction := trivial scope_d_gt_three_is_open := trivialThe graph of legal recognition events is the hypercube, derived from ledger atomicity rather than stipulated. t10HypercubeSubstrateCert · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.leanTHEOREM card_directedHypercubeEdges · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
lemma card_directedHypercubeEdges (d : Nat) : (directedHypercubeEdges d).card = d * 2 ^ d := by classical have hpart : (directedHypercubeEdges d).card = ∑ p : Pattern d, ((directedHypercubeEdges d).filter (fun e => e.1 = p)).card := by simpa [directedHypercubeEdges] using (Finset.card_eq_sum_card_fiberwise (s := directedHypercubeEdges d) (f := Prod.fst) (t := Finset.univ) (fun _ _ => Finset.mem_univ _)) refine hpart.trans ?_ have hfiber (p : Pattern d) : ((directedHypercubeEdges d).filter (fun e => e.1 = p)).card = d := by let N := Finset.univ.filter (fun q : Pattern d => HypercubeAdj p q) have hset : (directedHypercubeEdges d).filter (fun e => e.1 = p) = N.image (fun q => (p, q)) := by ext e constructor · intro he rcases Finset.mem_filter.mp he with ⟨he', hp⟩ rcases Finset.mem_filter.mp he' with ⟨_, hadj⟩ exact Finset.mem_image.mpr ⟨e.2, by simp [N, hp ▸ hadj], Prod.ext hp.symm rfl⟩ · intro he rcases Finset.mem_image.mp he with ⟨q, hq, rfl⟩ simp only [Finset.mem_filter, Finset.mem_univ, true_and, N] at hq exact Finset.mem_filter.mpr ⟨Finset.mem_filter.mpr ⟨Finset.mem_univ _, hq⟩, rfl⟩ have hinj : Set.InjOn (fun q : Pattern d => (p, q)) N := by intro _ _ _ _ h; exact (Prod.mk.inj h).2 rw [hset, Finset.card_image_of_injOn hinj, card_neighbors] simp_rw [hfiber] simp [Finset.sum_const, Patterns.card_pattern, Nat.mul_comm]A d-dimensional hypercube has d times 2 to the power (d minus 1) undirected edges. card_directedHypercubeEdges · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.leanTHEOREM hypercubeCut_le_total · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
/-- H5 ceiling. -/ theorem hypercubeCut_le_total {d : Nat} (A : Finset (Pattern d)) : hypercubeCut A ≤ d * 2 ^ (d - 1) := by classical cases d with | zero => have hz : hypercubeCut A = 0 := by unfold hypercubeCut refine Finset.card_eq_zero.mpr ?_ ext e simp only [Finset.notMem_empty, iff_false, Finset.mem_filter, Finset.mem_univ, true_and, HypercubeAdj] intro h -- no edges when there are no coordinates have : (Finset.univ : Finset (Fin 0)).card = 0 := by simp have hle := Finset.card_filter_le (s := (Finset.univ : Finset (Fin 0))) (p := fun i => e.1 i ≠ e.2 i) omega simp [hz] | succ d' => have hdir := card_directedHypercubeEdges (d' + 1) -- cut A ≤ half of directed edges via cut A = cut Aᶜ let Cut := Finset.univ.filter fun e : Pattern (d'+1) × Pattern (d'+1) => HypercubeAdj e.1 e.2 ∧ e.1 ∈ A ∧ e.2 ∉ A let Cut' := Finset.univ.filter fun e : Pattern (d'+1) × Pattern (d'+1) => HypercubeAdj e.1 e.2 ∧ e.1 ∉ A ∧ e.2 ∈ A let swapE := fun e : Pattern (d'+1) × Pattern (d'+1) => (e.2, e.1) have himage : Cut.image swapE = Cut' := by ext e constructor · intro he rcases Finset.mem_image.mp he with ⟨e', he', rfl⟩ rcases Finset.mem_filter.mp he' with ⟨_, hadj, hA, hnA⟩ exact Finset.mem_filter.mpr ⟨Finset.mem_univ _, hypercubeAdj_symm hadj, hnA, hA⟩ · intro he rcases Finset.mem_filter.mp he with ⟨_, hadj, hnA, hA⟩ exact Finset.mem_image.mpr ⟨(e.2, e.1), Finset.mem_filter.mpr ⟨Finset.mem_univ _, hypercubeAdj_symm hadj, hA, hnA⟩, rfl⟩ have hinj : Set.InjOn swapE Cut := by intro x _ y _ h; exact Prod.ext (Prod.mk.inj h).2 (Prod.mk.inj h).1 have hcuts : Cut.card = Cut'.card := by have := congrArg Finset.card himage rwa [Finset.card_image_of_injOn hinj] at this have hdisj : Disjoint Cut Cut' := by refine Finset.disjoint_left.mpr ?_ intro e he1 he2 exact (Finset.mem_filter.mp he2).2.2.1 (Finset.mem_filter.mp he1).2.2.1 have hsub : Cut ∪ Cut' ⊆ directedHypercubeEdges (d'+1) := by intro e he simp only [Finset.mem_union, Cut, Cut', Finset.mem_filter, directedHypercubeEdges] at he ⊢ rcases he with ⟨_, hadj, _, _⟩ | ⟨_, hadj, _, _⟩ <;> exact ⟨Finset.mem_univ _, hadj⟩ have hle : 2 * Cut.card ≤ (directedHypercubeEdges (d'+1)).card := by have := Finset.card_le_card hsub have hu := Finset.card_union_of_disjoint hdisj have : Cut.card + Cut'.card ≤ (directedHypercubeEdges (d'+1)).card := by simpa [hu] using this simpa [two_mul, hcuts] using this have : Cut.card ≤ (d'+1) * 2 ^ d' := by have h2 : 2 * Cut.card ≤ (d'+1) * 2 ^ (d'+1) := by simpa [hdir] using hle have hpow : (d'+1) * 2 ^ (d'+1) = 2 * ((d'+1) * 2 ^ d') := by rw [pow_succ]; ring have h2' : 2 * Cut.card ≤ 2 * ((d'+1) * 2 ^ d') := by simpa [hpow] using h2 exact Nat.le_of_mul_le_mul_left h2' (by decide : 0 < 2) simpa [hypercubeCut, Cut] using thisThe wall is an upper bound on what a substrate can support; it does not predict any particular mass. hypercubeCut_le_total · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.leanTHEOREM tau_ratio_forces_accounts · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
theorem tau_ratio_forces_accounts {d : Nat} (h : (347723 : ℚ) / 100 ≤ (2 : ℚ) ^ (d - 1)) : 13 ≤ d := by by_contra hlt; push_neg at hlt; interval_cases d <;> norm_num at hThe dimension d is not derived; the library only proves lower bounds from measured lepton ratios. tau_ratio_forces_accounts · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean