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lemma proved term proof high

phaseCharacter_zero

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The phase character of the zero displacement on any coupled ququart configuration equals unity. Researchers building tensor-Weyl monomials in the Recognition Science foundation cite this to reduce the identity case. The proof is a direct simplification of the product definition when the first configuration argument is zero.

claimFor any natural number $N$ and any configuration $s : (Fin N) → (Fin 4)$, the phase character of the zero configuration and $s$ equals $1$, where the phase character is the product over sites $x$ of $i$ raised to the product of the ququart values of the two configurations at $x$.

background

CoupledCoreIndex N is the type Fin N → Fin 4, the finite-site configuration space of coupled ququart cores that serves as the concrete Hilbert carrier. The phaseCharacter function maps a pair of such configurations to a complex number via the product over all sites of i to the power of the product of their ququart values. This lemma sits in the CoupledRecognitionCores module that assembles the basic operators on these carriers.

proof idea

The proof is a one-line wrapper that applies the definition of phaseCharacter and reduces the product to 1 when the displacement configuration is identically zero.

why it matters in Recognition Science

This lemma supplies the zero case needed by tensorWeylMonomial_zero_zero, which establishes that the trivial Weyl monomial acts as the identity operator on the coupled-core space. It closes the base case in the phase-character construction for tensor-Weyl expansions inside the foundation layer.

scope and limits

Lean usage

ext ψ s; simp [tensorWeylMonomial, phaseCharacter_zero, shiftedConfig_zero]

formal statement (Lean)

 140lemma phaseCharacter_zero {N : ℕ} (s : CoupledCoreIndex N) :
 141    phaseCharacter 0 s = 1 := by

proof body

Term-mode proof.

 142  simp [phaseCharacter]
 143
 144/-- Zero displacement leaves a coupled-core configuration unchanged. -/

used by (1)

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depends on (3)

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