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Projector-energy stationarity is equivalent to Fock commutation

Statement

Let E and F(P)=∇E(P) be the finite-basis model and gradient of Finite-basis projector energy model. A projector P∈Pr is stationary for E restricted to Pr—meaning DE(P)[H]=0 for every H∈TPPr—if and only if [F(P),P]:=F(P)P−PF(P)=0. Stationarity is only a first-order condition; it does not assert that P is a minimum.

Facts & Assumptions

Given: A C2 finite-basis projector energy, P∈Pr, and the real Frobenius inner product on Hermitian matrices.

[F1]

The Hermitian Frobenius gradient satisfies DE(P)[H]=tr⁡(F(P)H) for Hermitian H (The finite projector energy is real and has the stated Frobenius gradient).

[F2]

The tangent directions at P are exactly [K,P] for skew-Hermitian K, and each is the velocity of a feasible unitary-conjugation curve (Complex projector tangents are skew-Hermitian commutator directions).

Proof

1.1F1F2givenalgebra

Let K∗=−K. By [F2], HK=[K,P] is the velocity at zero of a feasible curve through P. The gradient formula [F1] gives DE(P)[HK]=tr⁡(F(P)(KP−PK)). Cyclicity of trace, which follows from tr⁡(AB)=∑i,jAijBji=tr⁡(BA), rewrites this as −tr⁡([F(P),P]K).

2.1F2step 1.1givenalgebra∎

Put C=[F(P),P]. Since F(P) and P are Hermitian, C∗=−C. If P is stationary, step 1.1 vanishes for every skew-Hermitian K; choosing K=C gives 0=−tr⁡(C2)=tr⁡(C∗C)=∥C∥F2, so C=0. Conversely, if C=0, step 1.1 vanishes for every K, and [F2] says these are all tangent directions, so P is stationary.

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