Encyclopedia Foundation Foundation Pair Kernel Exact Jevent Interaction Dual Event On Shell Iff Legendre
ARTICLE 3 claims 3 theorems
Foundation Pair Kernel Exact Jevent Interaction Dual Event On Shell Iff Legendre
A field configuration is physical exactly when it makes a certain bookkeeping expression stationary, a theorem that connects two ways of describing the same thing.
The on-shell condition
In classical physics, a system is said to be on shell when it satisfies the equations of motion, as opposed to being an arbitrary trial configuration. The Recognition Science declaration eventOnShell_iff_legendreCritical proves an equivalence: a field is on shell if and only if it is a critical point of a particular Legendre functional, which is an expression built from a source-field pairing minus an action term. This is a standard variational principle, familiar from classical mechanics where the path taken by a particle is the one that makes the action stationary.
The setting is a discrete one. The framework works with a finite set of points on a torus, and each field assigns a real number to each point. The source is an integer-valued discrete-Gauss profile representing a posting event. The declaration shows that the condition of being on shell, defined through a stationary condition, is exactly equivalent to the field satisfying a nonlinear Gauss equation pointwise. This means the two descriptions, one variational and one differential, pick out the same set of physical fields.
What makes this useful is that it allows two posting sources to be compared through their on-shell dual values without introducing a kinetic scale, a Born coupling, a field normalization, or a molecular Hamiltonian. The framework's library proves this as a theorem, with no axioms beyond the standard three and no empirical constants. The unit source pairing is a convention at the q=1 event lattice, and the exact-J cost does not select a dimensioned physical source scale.
The declaration does not claim that such on-shell fields exist or are unique for a given source, nor does it identify them with molecular binding. Those questions remain open. It also does not claim that the Legendre functional is the only way to characterize on-shell fields, only that this particular equivalence holds in this discrete setting.
THEOREM eventOnShell_iff_legendreCritical · IndisputableMonolith/Foundation/PairKernelExactJEventInteractionDual.lean
theorem eventOnShell_iff_legendreCritical
(source field : DualEventField3) :
IsExactJEventOnShell3 source field ↔
∀ variation,
eventSourcePairing3 source variation -
exactJFirstVariationPairing
eventInteractionGraph3 field variation = 0 := by
unfold IsExactJEventOnShell3 ExactJStationaryAtSource
constructor
· intro h variation
specialize h variation
simp only [one_mul] at h
rw [eventSourcePairing3_comm_sum]
linarith
· intro h variation
specialize h variation
rw [eventSourcePairing3_comm_sum] at h
simp only [one_mul]
linarith
THEOREM eventOnShell_iff_nonlinearGauss · IndisputableMonolith/Foundation/PairKernelExactJEventInteractionDual.lean
theorem eventOnShell_iff_nonlinearGauss
(source field : DualEventField3) :
IsExactJEventOnShell3 source field ↔
ExactJNonlinearGaussEquation
eventInteractionGraph3 field source 1 :=
exactJStationaryAtSource_iff_gauss
eventInteractionGraph3 field source 1
THEOREM exactJEventInteractionDual_cert · IndisputableMonolith/Foundation/PairKernelExactJEventInteractionDual.lean
theorem exactJEventInteractionDual_cert
(cfg : ExactJTwoEventConfig3) :
ExactJEventInteractionDualCert3 cfg where
source_neutral := compositeSource_sum_zero cfg
line_derivative :=
exactJEventLegendreFunctional3_hasDerivAt_line cfg.compositeSource
onShell_iff_gauss :=
eventOnShell_iff_nonlinearGauss cfg.compositeSource
gauge_invariant :=
compositeLegendreFunctional_gauge_invariant cfg
What this page does not claim
Existence or uniqueness of on-shell fields for a given source. Identification of on-shell fields with molecular binding. That the Legendre functional is the only characterization of on-shell fields. Selection of a dimensioned physical source scale by the exact-J cost.
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/PairKernelExactJEventInteractionDual.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 conditions guarantee existence and uniqueness of nonlinear on-shell fields?
- How does the discrete on-shell condition relate to the continuum notion from classical field theory?
- What physical interpretation, if any, attaches to the dual values of two posting sources?
- Does the equivalence extend to other source profiles beyond the unit posting source?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM eventOnShell_iff_legendreCritical · IndisputableMonolith/Foundation/PairKernelExactJEventInteractionDual.lean
theorem eventOnShell_iff_legendreCritical (source field : DualEventField3) : IsExactJEventOnShell3 source field ↔ ∀ variation, eventSourcePairing3 source variation - exactJFirstVariationPairing eventInteractionGraph3 field variation = 0 := by unfold IsExactJEventOnShell3 ExactJStationaryAtSource constructor · intro h variation specialize h variation simp only [one_mul] at h rw [eventSourcePairing3_comm_sum] linarith · intro h variation specialize h variation rw [eventSourcePairing3_comm_sum] at h simp only [one_mul] linarithA field is on shell if and only if it is a critical point of a particular Legendre functional. eventOnShell_iff_legendreCritical · IndisputableMonolith/Foundation/PairKernelExactJEventInteractionDual.leanTHEOREM eventOnShell_iff_nonlinearGauss · IndisputableMonolith/Foundation/PairKernelExactJEventInteractionDual.lean
theorem eventOnShell_iff_nonlinearGauss (source field : DualEventField3) : IsExactJEventOnShell3 source field ↔ ExactJNonlinearGaussEquation eventInteractionGraph3 field source 1 := exactJStationaryAtSource_iff_gauss eventInteractionGraph3 field source 1The on-shell condition is exactly equivalent to the field satisfying a nonlinear Gauss equation pointwise. eventOnShell_iff_nonlinearGauss · IndisputableMonolith/Foundation/PairKernelExactJEventInteractionDual.leanTHEOREM exactJEventInteractionDual_cert · IndisputableMonolith/Foundation/PairKernelExactJEventInteractionDual.lean
theorem exactJEventInteractionDual_cert (cfg : ExactJTwoEventConfig3) : ExactJEventInteractionDualCert3 cfg where source_neutral := compositeSource_sum_zero cfg line_derivative := exactJEventLegendreFunctional3_hasDerivAt_line cfg.compositeSource onShell_iff_gauss := eventOnShell_iff_nonlinearGauss cfg.compositeSource gauge_invariant := compositeLegendreFunctional_gauge_invariant cfgThe framework's library proves this as a theorem, with no axioms beyond the standard three and no empirical constants. exactJEventInteractionDual_cert · IndisputableMonolith/Foundation/PairKernelExactJEventInteractionDual.lean