IndisputableMonolith.Gravity.SevenGaps.HKTPointSplitStrong
Defines the strong point-split Hojman–Kuchař–Teitelboim dynamic target on a discrete circle, with Kronecker site weights and explicit Hamiltonian advection maps. Gravity gap-5 workers cite it to inhabit the n=2 strong target via a balanced quartic density and to refute strong rigidity. The module is mostly definitions plus elementary ZMod-2 arithmetic identities that pin the advection equalities.
claimOn $\mathbb{Z}/n\mathbb{Z}$, introduce the Kronecker site weight $\delta_i(j)$ (1 at $i$, 0 elsewhere), the computed Hamiltonian advection maps from/to a site, and the strong point-split HKT dynamic target structure. At $n=2$ these specialize with $\mathbb{Z}/2\mathbb{Z}$ successor identities and a balanced quartic Hamiltonian density used to inhabit the strong target.
background
Recognition Science gap-5 work reconstructs continuum constraint algebra in a discrete Hojman–Kuchař–Teitelboim (HKT) setting. The upstream point-split target module widens the dynamic HKT interface so momentum–Hamiltonian coupling is split across neighboring sites: an unsplit mom_ham field is uninhabitable for honest nearest-neighbor momentum against a frozen quadratic Hamiltonian, because at $n=2$ unsplit advection forces a singular identity when $p_0+p_1=0$.
This module supplies the strong variant of that point-split interface. The Kronecker lapse/shift weight on $\mathbb{Z}/n\mathbb{Z}$ marks a single site; computed advection maps package the discrete Hamiltonian flux from and to a site. Sibling lemmas record that the weight is 1 on the diagonal and 0 off it, and that the named advection fields equal those computed maps. At $n=2$, elementary $\mathbb{Z}/2\mathbb{Z}$ facts (successor never equals the base point; $0+1=1$, $1+1=0$) close the arithmetic.
proof idea
Definition-heavy module, not a single theorem campaign. Site weights are introduced as Kronecker indicators on $\mathbb{Z}/n\mathbb{Z}$, with immediate self/off-diagonal evaluations. Advection-from and advection-to are defined by explicit formulas and then identified with the structure fields of the strong target by rewriting. The $n=2$ layer is pure finite-ring arithmetic: successor inequalities and the two addition tables for $\mathbb{Z}/2\mathbb{Z}$. The strong target structure and the balanced quartic Hamiltonian density are packaged as named definitions for downstream inhabitation, not proved as existence theorems here.
why it matters in Recognition Science
Feeds the gap-5 rigidity kill and the constraint-recovery close path. Downstream HKTCanonicalMomTarget states the binding design: Session A inhabits the strong point-split target at $n=2$ by the balanced quartic falsifier and proves negation of the strong point-split rigidity statement; Session B then installs the repaired canonical-momentum class. Gap5ConstraintCloseStatus binds ledger flags so gap-5 constraint recovery reads closed and the continuum-algebra/HKT-open bits flip false, without import cycles through the full theory ledger. The audit module re-exports this surface for campaign checks. In the Seven Gaps gravity stack this is the strong-target carrier that lets the point-split repair actually host a smooth nearest-neighbor witness the unsplit frozen quadratic could not.
scope and limits
- Does not prove existence of a physical continuum limit or recover full GR constraint algebra.
- Does not inhabit the strong target; inhabitation and rigidity negation live downstream.
- Does not repair or replace the unsplit frozen-quadratic mom_ham pathology by itself.
- Does not claim the quartic density is the unique or observationally selected Hamiltonian.
- Does not address n≠2 geometry beyond the generic ZMod n weight definitions.
used by (3)
depends on (1)
declarations in this module (38)
-
def
siteDelta -
lemma
siteDelta_self -
lemma
siteDelta_ne -
def
computedHamAdvFrom -
def
computedHamAdvTo -
lemma
zmod2_succ_ne -
lemma
zmod2_zero_add_one' -
lemma
zmod2_one_add_one' -
theorem
hamAdvFrom_eq_computed -
theorem
hamAdvTo_eq_computed -
structure
HKTPointSplitTargetDynStrong -
def
quarticHamDensity2 -
def
zeroMomDensity2 -
def
decorativeStructure2 -
def
quarticHam2 -
def
quarticHam2D -
lemma
hasFDerivAt_quarticHam2 -
theorem
differentiable_quarticHam2 -
lemma
pderivQ_quarticHam2 -
theorem
bracket_quarticHam2_quarticHam2 -
lemma
zeroMom2_eq_zero -
lemma
differentiable_zeroMom2 -
lemma
bracket_zeroMom2_any -
lemma
decorativeStructure2_not_constant -
def
quarticNondegPhase -
theorem
quarticHamDensity2_nondeg -
def
quarticZeroMomTarget -
theorem
quarticZeroMomTarget_mom_vanishes -
theorem
quarticZeroMom_fails_mom_load_bearing -
theorem
quarticZeroMomTarget_not_strong -
def
momLoadBearingWitnessPhase -
lemma
momLoadBearingWitness_vals -
theorem
hamDyn_mom_load_bearing_witness -
theorem
hamDyn_kinetic_regular_witness -
def
hamDynPointSplitTargetStrong -
theorem
hktPointSplitTargetDynStrong_two_nonvacuous -
theorem
strong_target_discriminates_decoy -
def
HKTRigidityStatementPointSplitDynN2Strong