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inflatonPotential

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The inflaton potential is identified with the J-cost function J(φ) for φ > 0. Cosmologists modeling early-universe expansion inside Recognition Science would cite this identification when computing slow-roll parameters from the recognition composition law. The definition is a direct alias to the Jcost primitive with no further reduction.

claimThe inflaton potential $V(φ)$ for $φ > 0$ is given by $V(φ) = J(φ)$, where $J(φ) = (φ + φ^{-1})/2 - 1$.

background

The Cosmology.Inflation module derives cosmic inflation from J-cost slow roll. The J-cost is the function $J(x) = (x + x^{-1})/2 - 1$, which satisfies the recognition composition law $J(xy) + J(x/y) = 2J(x)J(y) + 2J(x) + 2J(y)$ and attains its global minimum of zero at $x = 1$. Near the minimum the potential is parabolic; far away it grows linearly, producing a flat region suitable for slow roll.

proof idea

One-line definition that directly aliases the Jcost function imported from the Cost module.

why it matters in Recognition Science

This supplies the potential $V(φ)$ used by the downstream theorems potential_min_at_one, potential_positive, slowRollEpsilon, slowRollEta and powerSpectrum. It realizes the module claim that inflation emerges from J-cost slow roll and thereby addresses the horizon, flatness and monopole problems. The construction sits inside the T5 J-uniqueness step of the forcing chain.

scope and limits

Lean usage

theorem potential_positive (φ : ℝ) (hφ : φ > 0) (hne : φ ≠ 1) : inflatonPotential φ hφ > 0 := by unfold inflatonPotential; exact Cost.Jcost_pos_of_ne_one φ hφ hne

formal statement (Lean)

  48noncomputable def inflatonPotential (φ : ℝ) (hφ : φ > 0) : ℝ := Jcost φ

proof body

Definition body.

  49
  50/-- **THEOREM**: The potential has a minimum at φ = 1. -/

used by (5)

From the project-wide theorem graph. These declarations reference this one in their body.

depends on (1)

Lean names referenced from this declaration's body.