Start here: KSW physics assessment and complete conditional specification

Resummation, Unitarity and Expansion Error

Why infinitely many leading bubbles, but only one derivative insertion at the first correction?

Definitions and assumptions

Scope and physical limitations

The primary theorem exhibits one nonempty momentum window in which every comparable subtraction scale has a failed raw leading-loop expansion and a small dressed first correction. The same observable matching fixes running contacts and actual beta derivatives; no assigned contact orders are assumed. The statement retains unique numerical solutions of the local PDS equations, the two amplitudes, leading and linearized unitarity, the optical defect and every finite-loop error. The five-field running data are its only project-defined object. The physical identification of this scalar model and the PDS calculation remains external; the precision bound is not an EFT remainder estimate. Earlier complete contracts, finite-chain arguments and treatment interpretation remain supporting roots without losing outputs. The higher-term polynomial diagnostic is not a realization by a finite-range nuclear potential.

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Examples and distinctions

Constructed examples of this model; each answer includes the Lean statement.

Exact root statement

∀ (flow : PhysicsLogic.Papers.KaplanSavageWise1998.PionlessRGFlow) (phase : ℝ → ℝ) (cutoff bound rho c epsilon : ℝ),
  0 < flow.mass →
    Filter.Tendsto (fun q => (phase q - -flow.inverseScatteringLength) / q ^ 2) (nhdsWithin 0 (Set.Ioi 0))
        (nhds (flow.effectiveRange / 2)) →
      (∀ (mu : ℝ),
          -mu + flow.inverseScatteringLength ≠ 0 →
            Filter.Tendsto (fun q => (-1 / (phase q + mu) - flow.mass / (4 * Real.pi) * flow.c0 mu) / q ^ 2)
              (nhdsWithin 0 (Set.Ioi 0)) (nhds (flow.mass / (4 * Real.pi) * flow.c2 mu))) →
        0 < cutoff →
          |cutoff * (flow.effectiveRange / 2)| ≤ bound →
            0 < rho →
              1 ≤ c →
                rho ^ 2 + 2 * c * rho ≤ 1 →
                  0 < epsilon →
                    epsilon < 1 →
                      |flow.inverseScatteringLength| * (bound + 1) < rho * epsilon * cutoff →
                        (∀ (mu : ℝ),
                            -mu + flow.inverseScatteringLength ≠ 0 →
                              flow.c0 mu = 4 * Real.pi / flow.mass * (-mu + flow.inverseScatteringLength)⁻¹ ∧
                                flow.c2 mu =
                                    2 * Real.pi / flow.mass * (-mu + flow.inverseScatteringLength)⁻¹ ^ 2 *
                                      flow.effectiveRange ∧
                                  HasDerivAt flow.c0 (flow.mass / (4 * Real.pi) * flow.c0 mu ^ 2) mu ∧
                                    HasDerivAt flow.c2 (flow.mass / (2 * Real.pi) * flow.c0 mu * flow.c2 mu) mu) ∧
                          (∃ p mu,
                              |flow.inverseScatteringLength| / rho < p ∧
                                p < epsilon * cutoff / (bound + 1) ∧ p ≤ c * mu ∧ mu ≤ c * p) ∧
                            ∀ (p mu : ℝ),
                              |flow.inverseScatteringLength| / rho < p →
                                p < epsilon * cutoff / (bound + 1) →
                                  p ≤ c * mu →
                                    mu ≤ c * p →
                                      -mu + flow.inverseScatteringLength ≠ 0 ∧
                                        have g0 := flow.mass / (4 * Real.pi) * flow.c0 mu;
                                        have g2 := flow.mass / (4 * Real.pi) * flow.c2 mu;
                                        (∃! pair,
                                            pair.1 + ↑g0 * (↑mu + Complex.I * ↑p) * pair.1 = -↑g0 ∧
                                              pair.2 + ↑g0 * (↑mu + Complex.I * ↑p) * pair.2 =
                                                -↑(g2 * p ^ 2) * (1 + (↑mu + Complex.I * ↑p) * pair.1)) ∧
                                          ∀ (leading correction : ℂ),
                                            leading + ↑g0 * (↑mu + Complex.I * ↑p) * leading = -↑g0 ∧
                                                correction + ↑g0 * (↑mu + Complex.I * ↑p) * correction =
                                                  -↑(g2 * p ^ 2) * (1 + (↑mu + Complex.I * ↑p) * leading) →
                                              leading = (-↑flow.inverseScatteringLength - Complex.I * ↑p)⁻¹ ∧
                                                correction = -↑(flow.effectiveRange / 2 * p ^ 2) * leading ^ 2 ∧
                                                  ‖correction‖ ≤ bound * p / cutoff * ‖leading‖ ∧
                                                    ‖correction‖ < epsilon * ‖leading‖ ∧
                                                      ‖correction‖ < ‖leading‖ ∧
                                                        Complex.normSq (1 + 2 * Complex.I * ↑p * leading) = 1 ∧
                                                          correction.im = 2 * p * (star leading * correction).re ∧
                                                            (∀ (t : ℝ),
                                                                (leading + ↑t * correction).im -
                                                                    p * Complex.normSq (leading + ↑t * correction) =
                                                                  -p * t ^ 2 * Complex.normSq correction) ∧
                                                              ∀ (n : ℕ),
                                                                have loopSum :=
                                                                  ∑ j ∈ Finset.range (n + 1),
                                                                    -↑g0 * (-↑g0 * (↑mu + Complex.I * ↑p)) ^ j;
                                                                ‖loopSum - leading‖ =
                                                                    (|g0| * ‖↑mu + Complex.I * ↑p‖) ^ (n + 1) *
                                                                      ‖leading‖ ∧
                                                                  ‖leading‖ ≤ ‖loopSum - leading‖
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  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary
  • external type boundary