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Variational ground gap overlap

Statement

Assume the Axiom of Choice and the Axiom of Countable Choice (The Axiom of Choice, The Axiom of Countable Choice (ACω)). Let H be a self-adjoint operator on a nonzero complex Hilbert space H (Symmetric, self-adjoint and essentially self-adjoint operators, Hilbert space) which is bounded below, let E0:=inf⁡σ(H)∈R, let E be the projection-valued measure of H (Spectral theorem for unbounded self-adjoint operators (PVM form), Projection valued measure), put P:=E({E0}), and assume that g>0 is a spectral gap: σ(H)∩(E0,E0+g)=∅. For u∈D(∣H∣1/2) write Eu(B):=⟨E(B)u,u⟩ for Borel sets B⊆R (Scalar and complex measures from a pvm) and put qH[u]:=∫Rλ dEu(λ); by Density operators and scalar spectral probability (c) this integral exists for u∈D(∣H∣1/2), and for u∈D(H) it equals ⟨Hu,u⟩. Then for every u∈D(∣H∣1/2) with ∥u∥=1:

(a) qH[u]−E0=∫R(λ−E0) dEu(λ) ≥ g ∥(I−P)u∥2;

(b) if qH[u]≤E0+ε for some ε≥0, then ∥(I−P)u∥2≤ε/g; in particular, if ε<g then Pu≠0.

No claim is made about the existence of a ground eigenvector, about E0 being an eigenvalue, or about any physical interpretation of the trial vector.

Facts & Assumptions

Given: the self-adjoint operator H bounded below with bottom E0=inf⁡σ(H), its projection-valued measure E, the ground projection P=E({E0}), a gap g>0, and a vector u∈D(∣H∣1/2) with ∥u∥=1.

[F1]

For a self-adjoint H and unit u∈D(∣H∣1/2), the scalar measure Eu(B)=⟨E(B)u,u⟩ is a probability measure and ∫∣λ∣ dEu<∞, so its signed first moment ∫λ dEu is finite; if u∈D(H), that moment equals ⟨Hu,u⟩ (Density operators and scalar spectral probability (c), Scalar and complex measures from a pvm, Spectral theorem for unbounded self-adjoint operators (PVM form)). No square-root expectation of H is asserted when H may have negative spectrum.

[F2]

E({E0})=P is an orthogonal projection; for every Borel set B, Eu(B)=∥E(B)u∥2, and E(B)=0 implies Eu(B)=0 (Projection valued measure).

[F3]

E0=inf⁡σ(H) means σ(H)⊆[E0,∞), so E((−∞,E0))=0; the gap hypothesis means E((E0,E0+g))=0 (Spectral theorem for unbounded self-adjoint operators (PVM form), Projection valued measure, Symmetric, self-adjoint and essentially self-adjoint operators).

Proof

1.1F1F2F3algebra

[Support of the scalar measure] By [F2] and [F3], Eu((−∞,E0))=∥E((−∞,E0))u∥2=0 and Eu((E0,E0+g))=∥E((E0,E0+g))u∥2=0; hence Eu is concentrated on {E0}∪[E0+g,∞) and, since Eu is a probability measure ([F1]), Eu(R)=∥u∥2=1, Eu({E0})=∥Pu∥2 and Eu([E0+g,∞))=∥(I−P)u∥2.

2.1F1step 1.1algebra

[The first-moment inequality] Write (λ−E0)+:=(λ−E0)1[E0,∞)(λ), a nonnegative Borel function equal to λ−E0 on the support of Eu by step 1.1. Since ∫∣λ∣ dEu<∞ by [F1] and Eu(R)=1, ∫(λ−E0) dEu=∫λ dEu−E0=qH[u]−E0. On the support, (λ−E0)+≥g 1[E0+g,∞)(λ), so qH[u]−E0≥g Eu([E0+g,∞))=g∥(I−P)u∥2, which is (a); if in addition qH[u]≤E0+ε, then g∥(I−P)u∥2≤ε.

3.1step 2.1algebra∎

[Failure of the ground component] If ε<g, then ∥(I−P)u∥2≤ε/g<1=∥u∥2, so ∥Pu∥2=∥u∥2−∥(I−P)u∥2>0 and Pu≠0; this completes the proof of (b) and of the statement.

Depends on

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