Encyclopedia Masses Masses Mass Genesis T10 Hypercube Substrate Hypercube Edge Connectivity Three In
ARTICLE 4 claims 3 theorems 1 model
Masses Mass Genesis T10 Hypercube Substrate Hypercube Edge Connectivity Three In
A machine-checked proof shows that a three-dimensional hypercube graph cannot be split into two nonempty parts by cutting fewer than three edges.
The three-dimensional wall
A hypercube graph is a network whose vertices are strings of bits, with an edge between two vertices when they differ in exactly one bit. The three-dimensional hypercube is the familiar cube: eight vertices, each connected to three neighbors. Its edge connectivity is three, meaning that any way of dividing the eight vertices into two nonempty groups must cut at least three edges. The declaration hypercubeEdgeConnectivity_three_inhabited is a machine-checked proof of exactly this fact, established in the framework's library of formal theorems.
The proof is not a numerical check but a general argument. It shows that for any nonempty proper subset of the cube's vertices, the number of edges crossing from the subset to its complement is at least three. This is the classical edge-connectivity property of the cube, proved in full generality for the three-dimensional case. The same library carries the general statement for any dimension d, and the three-dimensional instance is discharged by a bipartite handshaking argument, not by exhaustive computation.
In Recognition Science, this graph appears as the substrate on which particle masses are modeled. The framework derives the substrate graph from ledger atomicity: legal posts to a discrete record of events induce a graph on parity patterns, and that graph is the hypercube. The three-dimensional case matters because mass-genesis modules use d = 3, giving a wall of four edges. The theorem establishes that this wall is real: no smaller cut can separate the substrate's states.
What the declaration does not claim is equally precise. It does not derive the dimension d itself; lower bounds on d come from measured lepton ratios, not from this theorem. It does not predict any particular mass value, since the wall is an upper bound on what the substrate can support, not a specific outcome. And it does not settle whether d greater than 3 is legitimate here; that question remains open in the framework.
THEOREM hypercubeEdgeConnectivity_three_inhabited · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
theorem hypercubeEdgeConnectivity_three_inhabited :
HypercubeEdgeConnectivity 3 :=
hypercubeEdgeConnectivity_three
THEOREM hypercubeEdgeConnectivity_three · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
theorem hypercubeEdgeConnectivity_three : HypercubeEdgeConnectivity 3 := by
intro A hne hneU
have hpos : 0 < A.card := Finset.card_pos.mpr hne
have hlt := card_lt_univ (d := 3) hneU
by_cases hbig : 5 ≤ A.card
· have hAc : (Aᶜ).card = 8 - A.card := by
simpa [Patterns.card_pattern] using Finset.card_compl A
have hAcpos : 0 < (Aᶜ).card := by omega
have hle : (Aᶜ).card ≤ 3 := by omega
have hge := hypercubeCut_ge_when_small (d := 3) Aᶜ hAcpos hle
have : 3 ≤ (Aᶜ).card * (3 + 1 - (Aᶜ).card) := by
interval_cases (Aᶜ).card <;> norm_num
have := le_trans this hge
simpa [hypercubeCut_compl A] using this
· push_neg at hbig
by_cases h4 : A.card = 4
· have hsum := degree_sum_eq_internal_plus_cut (d := 3) A
have hin := hypercubeInternalDir_le_parts (d := 3) A
set ae := (A.filter (fun p => hammingWeight p % 2 = 0)).card with hae
set ao := (A.filter (fun p => hammingWeight p % 2 = 1)).card with hao
have hsumparts : ae + ao = 4 := by
have hsplit :
A =
A.filter (fun p => hammingWeight p % 2 = 0) ∪
A.filter (fun p => hammingWeight p % 2 = 1) := by
ext p; simp; constructor
· intro hp; by_cases h : hammingWeight p % 2 = 0
· exact Or.inl ⟨hp, h⟩
· exact Or.inr ⟨hp, by omega⟩
· intro h; rcases h with ⟨hp, _⟩ | ⟨hp, _⟩ <;> exact hp
have hdisj :
Disjoint (A.filter (fun p => hammingWeight p % 2 = 0))
(A.filter (fun p => hammingWeight p % 2 = 1)) := by
refine Finset.disjoint_left.mpr ?_
intro p hp0 hp1
have h0 := (Finset.mem_filter.mp hp0).2
have h1 := (Finset.mem_filter.mp hp1).2
omega
have hcu := Finset.card_union_of_disjoint hdisj
have : ae + ao = A.card := by
rw [hae, hao, ← hcu, ← hsplit]
omega
have hprod : ae * ao ≤ 4 := by
have : ae ≤ 4 := by omega
interval_cases ae <;> omega
have hin' : hypercubeInternalDir A ≤ 2 * (ae * ao) := by
simpa [Nat.mul_assoc] using hin
have hle8 : hypercubeInternalDir A ≤ 8 :=
Nat.le_trans hin' (Nat.mul_le_mul_left 2 hprod)
have h12 : hypercubeCut A + hypercubeInternalDir A = 12 := by
have : 3 * A.card = 12 := by simp [h4]
omega
have : 4 ≤ hypercubeCut A := by omega
exact Nat.le_trans (by decide : 3 ≤ 4) this
· have hle : A.card ≤ 3 := by omega
have hge := hypercubeCut_ge_when_small (d := 3) A hpos hle
have : 3 ≤ A.card * (3 + 1 - A.card) := by
interval_cases A.card <;> norm_num
exact le_trans this hge
MODEL T10HypercubeSubstrateCert · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
structure T10HypercubeSubstrateCert : Prop where
oneBitDiff_iff_adj :
∀ {d : Nat} (p q : Pattern d), OneBitDiff p q ↔ HypercubeAdj p q
legal_tick_is_hypercube_edge :
∀ {d : Nat} {L L' : LedgerState d},
LegalAtomicTick L L' → HypercubeAdj (parity d L) (parity d L')
post_realizes_flip :
∀ {d : Nat} (L : LedgerState d) (k : Fin d) (side : Side),
HypercubeAdj (parity d L) (parity d (post L k side)) ∧
parity d (post L k side) = flipAt (parity d L) k
bipartite :
∀ {d : Nat} {p q : Pattern d},
HypercubeAdj p q → hammingWeight p % 2 ≠ hammingWeight q % 2
xor_preserves_adj :
∀ {d : Nat} (c : Pattern d) {p q : Pattern d},
HypercubeAdj p q → HypercubeAdj (xorBy c p) (xorBy c q)
xor_transitive :
∀ {d : Nat} (p q : Pattern d), ∃ c : Pattern d, xorBy c p = q
evenClass_attains_maxcut :
∀ d : Nat, 0 < d → hypercubeCut (evenClass d) = d * 2 ^ (d - 1)
singleton_cut_eq_degree :
∀ {d : Nat} (p : Pattern d), hypercubeCut ({p} : Finset (Pattern d)) = d
connectivity_three : HypercubeEdgeConnectivity 3
wall_three : hypercubeCut (evenClass 3) = 4 * 3
muon_forces_d : ∀ d : Nat,
(206768 : ℚ) / 1000 ≤ (2 : ℚ) ^ (d - 1) → 9 ≤ d
tau_forces_d : ∀ d : Nat,
(347723 : ℚ) / 100 ≤ (2 : ℚ) ^ (d - 1) → 13 ≤ d
muon_forces_cells : ∀ N : Nat,
(206768 : ℚ) / 1000 ≤ (2 : ℚ) ^ (3 * N - 1) → 3 ≤ N
tau_forces_cells : ∀ N : Nat,
(347723 : ℚ) / 100 ≤ (2 : ℚ) ^ (3 * N - 1) → 5 ≤ N
posting_witness :
let L := zeroLedger 3
let L' := post L (0 : Fin 3) Side.debit
LegalAtomicTick L L' ∧
HypercubeAdj (parity 3 L) (parity 3 L') ∧
parity 3 L' = flipAt (parity 3 L) 0
scope_does_not_derive_d : True
scope_wall_is_capacity_not_prediction : True
scope_d_gt_three_is_open : True
THEOREM muon_ratio_forces_accounts · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
theorem muon_ratio_forces_accounts {d : Nat}
(h : (206768 : ℚ) / 1000 ≤ (2 : ℚ) ^ (d - 1)) : 9 ≤ d := by
by_contra hlt; push_neg at hlt; interval_cases d <;> norm_num at h
What this page does not claim
The theorem does not derive the dimension d from ledger atomicity. It does not predict any particular particle mass value. It does not establish whether d greater than 3 is legitimate in the framework.
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 mechanism, if any, fixes the substrate dimension d at a value above three?
- How does the wall of four edges in three dimensions relate to the measured lepton mass ratios?
- What would a substrate with d greater than 3 imply for the mass-genesis modules that currently use d = 3?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM hypercubeEdgeConnectivity_three_inhabited · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
theorem hypercubeEdgeConnectivity_three_inhabited : HypercubeEdgeConnectivity 3 := hypercubeEdgeConnectivity_threeIts edge connectivity is three, meaning that any way of dividing the eight vertices into two nonempty groups must cut at least three edges. hypercubeEdgeConnectivity_three_inhabited · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.leanTHEOREM hypercubeEdgeConnectivity_three · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
theorem hypercubeEdgeConnectivity_three : HypercubeEdgeConnectivity 3 := by intro A hne hneU have hpos : 0 < A.card := Finset.card_pos.mpr hne have hlt := card_lt_univ (d := 3) hneU by_cases hbig : 5 ≤ A.card · have hAc : (Aᶜ).card = 8 - A.card := by simpa [Patterns.card_pattern] using Finset.card_compl A have hAcpos : 0 < (Aᶜ).card := by omega have hle : (Aᶜ).card ≤ 3 := by omega have hge := hypercubeCut_ge_when_small (d := 3) Aᶜ hAcpos hle have : 3 ≤ (Aᶜ).card * (3 + 1 - (Aᶜ).card) := by interval_cases (Aᶜ).card <;> norm_num have := le_trans this hge simpa [hypercubeCut_compl A] using this · push_neg at hbig by_cases h4 : A.card = 4 · have hsum := degree_sum_eq_internal_plus_cut (d := 3) A have hin := hypercubeInternalDir_le_parts (d := 3) A set ae := (A.filter (fun p => hammingWeight p % 2 = 0)).card with hae set ao := (A.filter (fun p => hammingWeight p % 2 = 1)).card with hao have hsumparts : ae + ao = 4 := by have hsplit : A = A.filter (fun p => hammingWeight p % 2 = 0) ∪ A.filter (fun p => hammingWeight p % 2 = 1) := by ext p; simp; constructor · intro hp; by_cases h : hammingWeight p % 2 = 0 · exact Or.inl ⟨hp, h⟩ · exact Or.inr ⟨hp, by omega⟩ · intro h; rcases h with ⟨hp, _⟩ | ⟨hp, _⟩ <;> exact hp have hdisj : Disjoint (A.filter (fun p => hammingWeight p % 2 = 0)) (A.filter (fun p => hammingWeight p % 2 = 1)) := by refine Finset.disjoint_left.mpr ?_ intro p hp0 hp1 have h0 := (Finset.mem_filter.mp hp0).2 have h1 := (Finset.mem_filter.mp hp1).2 omega have hcu := Finset.card_union_of_disjoint hdisj have : ae + ao = A.card := by rw [hae, hao, ← hcu, ← hsplit] omega have hprod : ae * ao ≤ 4 := by have : ae ≤ 4 := by omega interval_cases ae <;> omega have hin' : hypercubeInternalDir A ≤ 2 * (ae * ao) := by simpa [Nat.mul_assoc] using hin have hle8 : hypercubeInternalDir A ≤ 8 := Nat.le_trans hin' (Nat.mul_le_mul_left 2 hprod) have h12 : hypercubeCut A + hypercubeInternalDir A = 12 := by have : 3 * A.card = 12 := by simp [h4] omega have : 4 ≤ hypercubeCut A := by omega exact Nat.le_trans (by decide : 3 ≤ 4) this · have hle : A.card ≤ 3 := by omega have hge := hypercubeCut_ge_when_small (d := 3) A hpos hle have : 3 ≤ A.card * (3 + 1 - A.card) := by interval_cases A.card <;> norm_num exact le_trans this hgeThe three-dimensional instance is discharged by a bipartite handshaking argument, not by exhaustive computation. hypercubeEdgeConnectivity_three · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.leanMODEL T10HypercubeSubstrateCert · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
structure T10HypercubeSubstrateCert : Prop where oneBitDiff_iff_adj : ∀ {d : Nat} (p q : Pattern d), OneBitDiff p q ↔ HypercubeAdj p q legal_tick_is_hypercube_edge : ∀ {d : Nat} {L L' : LedgerState d}, LegalAtomicTick L L' → HypercubeAdj (parity d L) (parity d L') post_realizes_flip : ∀ {d : Nat} (L : LedgerState d) (k : Fin d) (side : Side), HypercubeAdj (parity d L) (parity d (post L k side)) ∧ parity d (post L k side) = flipAt (parity d L) k bipartite : ∀ {d : Nat} {p q : Pattern d}, HypercubeAdj p q → hammingWeight p % 2 ≠ hammingWeight q % 2 xor_preserves_adj : ∀ {d : Nat} (c : Pattern d) {p q : Pattern d}, HypercubeAdj p q → HypercubeAdj (xorBy c p) (xorBy c q) xor_transitive : ∀ {d : Nat} (p q : Pattern d), ∃ c : Pattern d, xorBy c p = q evenClass_attains_maxcut : ∀ d : Nat, 0 < d → hypercubeCut (evenClass d) = d * 2 ^ (d - 1) singleton_cut_eq_degree : ∀ {d : Nat} (p : Pattern d), hypercubeCut ({p} : Finset (Pattern d)) = d connectivity_three : HypercubeEdgeConnectivity 3 wall_three : hypercubeCut (evenClass 3) = 4 * 3 muon_forces_d : ∀ d : Nat, (206768 : ℚ) / 1000 ≤ (2 : ℚ) ^ (d - 1) → 9 ≤ d tau_forces_d : ∀ d : Nat, (347723 : ℚ) / 100 ≤ (2 : ℚ) ^ (d - 1) → 13 ≤ d muon_forces_cells : ∀ N : Nat, (206768 : ℚ) / 1000 ≤ (2 : ℚ) ^ (3 * N - 1) → 3 ≤ N tau_forces_cells : ∀ N : Nat, (347723 : ℚ) / 100 ≤ (2 : ℚ) ^ (3 * N - 1) → 5 ≤ N posting_witness : let L := zeroLedger 3 let L' := post L (0 : Fin 3) Side.debit LegalAtomicTick L L' ∧ HypercubeAdj (parity 3 L) (parity 3 L') ∧ parity 3 L' = flipAt (parity 3 L) 0 scope_does_not_derive_d : True scope_wall_is_capacity_not_prediction : True scope_d_gt_three_is_open : TrueIn Recognition Science, this graph appears as the substrate on which particle masses are modeled. T10HypercubeSubstrateCert · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.leanTHEOREM muon_ratio_forces_accounts · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean
theorem muon_ratio_forces_accounts {d : Nat} (h : (206768 : ℚ) / 1000 ≤ (2 : ℚ) ^ (d - 1)) : 9 ≤ d := by by_contra hlt; push_neg at hlt; interval_cases d <;> norm_num at hIt does not derive the dimension d itself; lower bounds on d come from measured lepton ratios, not from this theorem. muon_ratio_forces_accounts · IndisputableMonolith/Masses/MassGenesis/T10HypercubeSubstrate.lean