Eqs. (8)–(9): off the spectrum, a regular solution with exists
ProvedGiddings1999.nonNormalizable_mode_existsads-cftmathematical-physics
Let , , , , and let satisfy for every . Then there is a solution of the radial equation at frequency that is bounded near and satisfies
These are the non-normalizable modes of eq. (8), in the normalization convention of eq. (9).
Formalization Note The paper says these solutions exist "at arbitrary frequency". At the solution that is regular at is the normalizable , so the coefficient of cannot be normalized to . The statement therefore excludes the spectrum.
Preamble
import Mathlib import Definitions.Def_Giddings1999_AdSModes open Real Filter Topology
Formal statement
namespace Giddings1999
/-- **Milestone, eqs. (8), (9)**: away from the normalizable spectrum, there is a solution regular at
the origin with boundary behaviour `χ_{ωl}(r) → (cos r)^{2h₋}` (normalized coefficient `1`). -/
theorem nonNormalizable_mode_exists (d : ℕ) (hd : 2 ≤ d) (m R : ℝ) (hR : 0 < R) (ω : ℝ) (l : ℕ)
(hω : ∀ n : ℕ, |ω| ≠ omegaNL d m R n l) :
∃ χ : ℝ → ℝ, IsRadialSolution d m R ω l χ ∧ IsRegularAtOrigin χ ∧
Tendsto (fun r => χ r / cos r ^ twoHMinus d m R) (𝓝[<] (π / 2)) (𝓝 1) := by
sorry
end Giddings1999Source
S. B. Giddings, Boundary S matrix and the anti-de Sitter space to conformal field theory dictionary, Phys. Rev. Lett. 83, 2707 (1999), https://doi.org/10.1103/PhysRevLett.83.2707, eqs. (8), (9), p. 2707
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.