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Potentials in L∞∞+L2L^\infty_\infty + L^2L∞∞​+L2 are relatively compact with respect to H0H_0H0​

Proved
TeschlQM.OneParticle.potential_relativelyCompact

by Gabewhigham · Oct 7, 2026 · Mathlib 0df444a (Lean v4.33.1)

mathematical-physicsschrodinger-operatorsspectral-theory

Let n≥1n\ge1n≥1 and V:Rn→RV:\mathbb R^n\to\mathbb RV:Rn→R. Suppose V∈L∞∞(Rn)V\in L^\infty_\infty(\mathbb R^n)V∈L∞∞​(Rn) (bounded, Borel, vanishing at infinity) if n>3n>3n>3, and V∈L∞∞(Rn)+L2(Rn)V\in L^\infty_\infty(\mathbb R^n)+L^2(\mathbb R^n)V∈L∞∞​(Rn)+L2(Rn) if n≤3n\le3n≤3. Then the maximally defined multiplication operator VVV is relatively compact with respect to the free Schrödinger operator H0H_0H0​: there is z∈ρ(H0)z\in\rho(H_0)z∈ρ(H0​) with Ran⁡RH0(z)⊆D(V)\operatorname{Ran}R_{H_0}(z)\subseteq\mathfrak D(V)RanRH0​​(z)⊆D(V) and VRH0(z)V R_{H_0}(z)VRH0​​(z) compact.

This is the first assertion of Teschl's Theorem 10.2. Its proof combines Lemma 7.11 (for the L∞∞L^\infty_\inftyL∞∞​ part) with Lemma 10.1 (for the L2L^2L2 part, n≤3n\le 3n≤3).

Preamble
import Mathlib
import Definitions.Def_TeschlQM_OneParticle_multiplicationOperator
import Definitions.Def_TeschlQM_OneParticle_freeHamiltonian
import Definitions.Def_TeschlQM_Shared_resolventSet
import Definitions.Def_TeschlQM_Shared_IsRelativelyCompact
import Definitions.Def_TeschlQM_OneParticle_IsBoundedVanishingAtInfinity
Formal statement
namespace TeschlQM.OneParticle

open MeasureTheory

/-- Teschl, proof of Theorem 10.2, p. 222 (via Lemma 7.11 and Lemma 10.1): if `V ∈ L^∞_∞(ℝⁿ)`
for `n > 3` and `V ∈ L^∞_∞(ℝⁿ) + L²(ℝⁿ)` for `n ≤ 3`, then the multiplication operator `V` is
relatively compact with respect to the free Schrödinger operator `H₀`. -/
theorem potential_relativelyCompact (n : ℕ) (hn : 1 ≤ n) (V : EuclideanSpace ℝ (Fin n) → ℝ)
    (hV_large : 3 < n → IsBoundedVanishingAtInfinity V)
    (hV_small : n ≤ 3 → ∃ V₁ V₂ : EuclideanSpace ℝ (Fin n) → ℝ,
      IsBoundedVanishingAtInfinity V₁ ∧ MemLp V₂ 2 volume ∧ V = V₁ + V₂) :
    TeschlQM.Shared.IsRelativelyCompact (multOp (fun x => (V x : ℂ))) (freeHamiltonian n) := by
  sorry

end TeschlQM.OneParticle
Source
Teschl, Mathematical Methods in Quantum Mechanics, AMS GSM 99, 2009, Theorem 10.2 (p. 222), first assertion; proof via Lemma 7.11 (p. 170) and Lemma 10.1 (p. 221)

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