Three-state switch: norm and finite-volume spectral bounds
OpenUndecidableSpectralGap.usg_switch_finite_spectrummathematical-physicsquantum-informationspectral-gaptheoretical-computer-scienceundecidability
For positive b≤1/2 and |a|≤b, the three-state switch has local interaction strength at most one. For every L≥2, put E=aL². Its spectrum contains zero and E, is bounded below by min(0,E), and contains the translated row-magnon set:
If E≥1, zero has multiplicity one and all other eigenvalues are at least one. These finite-dimensional bounds are independent of any machine or halting predicate. The lower size cutoff excludes the empty lattice and the one-site graph.
Preamble
import Definitions.Def_usg_three_state_switch set_option autoImplicit false open UndecidableSpectralGap
Formal statement
theorem UndecidableSpectralGap.usg_switch_finite_spectrum
(b a : ℝ) (hb : 0 < b) (hbhalf : b ≤ 1 / 2) (ha : |a| ≤ b) :
localInteractionStrength ((a : ℂ) • switchProjector)
(switchGuard + (b : ℂ) • switchExchange) switchGuard ≤ 1 ∧
∀ L : ℕ, 2 ≤ L →
(0 ∈ specReal (switchHam L a b) ∧
a * (L : ℝ) ^ 2 ∈ specReal (switchHam L a b) ∧
∀ μ ∈ specReal (switchHam L a b), min 0 (a * (L : ℝ) ^ 2) ≤ μ) ∧
(∀ s ∈ switchMagnonSpectrum L b,
a * (L : ℝ) ^ 2 + s ∈ specReal (switchHam L a b)) ∧
(1 ≤ a * (L : ℝ) ^ 2 → eigMultiplicity (switchHam L a b) 0 = 1 ∧
∀ μ ∈ specReal (switchHam L a b), μ ≠ 0 → 1 ≤ μ) := by sorrySource
Original auxiliary specialization of the vacuum/occupied-sector construction in Cubitt–Pérez-García–Wolf, arXiv:1502.04573v5, Section 6.2, equations (130a)–(130d). The occupied row interaction is twice the spin-1/2 Hamiltonian of Napiórkowski–Seiringer, Free energy asymptotics of the quantum Heisenberg spin chain, https://doi.org/10.1007/s11005-021-01375-4, equation (2.1). This is a concrete auxiliary model, not a restatement of either paper’s undecidability theorem.