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Three-state switch contains the translated row-magnon spectrum

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UndecidableSpectralGap.usg_switch_magnon_inclusion

by Mazecto · Sep 22, 2026 · Mathlib 0df444a (Lean v4.33.1)

mathematical-physicsquantum-informationspectral-gap

Let 0<b≤1/20<b\le 1/20<b≤1/2, ∣a∣≤b|a|\le b∣a∣≤b, and L≥2L\ge2L≥2. Every sum sss of one-magnon path-Laplacian energies, with one independently chosen mode in each occupied row, produces an eigenvalue of the three-state switch Hamiltonian after adding the occupied-sector shift:

aL2+SL(b)⊆spec⁡RHL(a,b).aL^2+S_L(b)\subseteq\operatorname{spec}_{\mathbb R} H_L(a,b).aL2+SL​(b)⊆specR​HL​(a,b).

This isolates the tensor-product row-magnon construction used to populate the finite-volume spectrum.

Preamble
import Definitions.Def_usg_three_state_switch

set_option autoImplicit false
open UndecidableSpectralGap
Formal statement
theorem UndecidableSpectralGap.usg_switch_magnon_inclusion
    (b a : ℝ) (hb : 0 < b) (hbhalf : b ≤ 1 / 2) (ha : |a| ≤ b) :
    ∀ L : ℕ, 2 ≤ L →
      ∀ s ∈ switchMagnonSpectrum L b,
        a * (L : ℝ) ^ 2 + s ∈ specReal (switchHam L a b) := by sorry
Source
Original auxiliary specialization of the vacuum/occupied-sector construction in Cubitt–Pérez-García–Wolf, arXiv:1502.04573v5, Section 6.2, equations (130a)–(130d); one-row magnon energies follow Napiórkowski–Seiringer, doi:10.1007/s11005-021-01375-4, equation (2.1).

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