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Complex projector tangents are skew-Hermitian commutator directions

Statement

Let P∈Pr and define the tangent space by velocities of differentiable curves in Pr. Then TPPr={[K,P]:K∗=−K},[K,P]:=KP−PK. For each skew-Hermitian K, the curve can be realized near t=0 as PK(t)=QK(t)PQK(t)∗, where QK(t):=(I+tK/2)(I−tK/2)−1.

Facts & Assumptions

Given: P∈Pr in a finite-dimensional complex inner-product space and a skew-Hermitian matrix K∗=−K.

[F1]

The rank-r projector domain consists of Hermitian idempotents with trace r (Rank-r orthogonal projector domain).

[F2]

At P, the tangent directions are exactly the Hermitian off-diagonal blocks between range⁡P and its orthogonal complement; every such block is realized by the graph chart (Graph charts and tangent directions for complex rank-r projectors).

[F3]

The inner product is linear in its first argument, conjugate-linear in its second, and positive definite; the adjoint satisfies ⟨Ax,y⟩=⟨x,A∗y⟩ (Real and complex inner-product spaces and their induced length, The norm ∥v∥=⟨v,v⟩ induced by a real or complex inner product, The adjoint T∗:W→V is characterised by ⟨Tv,w⟩W=⟨v,T∗w⟩V).

[F4]

For a linear map on an n-dimensional space, dim⁡ker⁡T+dim⁡im⁡T=n (Rank-nullity: dim⁡FV=nullity⁡T+rank⁡T). A subspace of an n-dimensional space having dimension n equals the whole space (If dim⁡FV=n and U is a linear subspace of V, then U is finite-dimensional, dim⁡FU≤n, and dim⁡FU=n if and only if U=V, claim 2).

[F5]

Matrix inversion has derivative Dinv⁡(A)[H]=−A−1HA−1, and matrix differentials obey product and adjoint rules (On the invertible locus, Dinv⁡(A)[H]=−A−1HA−1, Matrix differentials obey the sum rule, product rule, and adjoint rule).

Proof

1.1F3F4givenalgebra

Put Mt=I−tK/2. If t≠0 and Mtx=0 for a nonzero x, then Kx=(2/t)x. By [F3], Re⁡⟨Kx,x⟩=0, while this equation gives ⟨Kx,x⟩=(2/t)∥x∥2, a nonzero real number. This contradiction shows ker⁡Mt={0}; M0=I is also injective. By [F4], dim⁡im⁡Mt=n, hence im⁡Mt=Cn. Thus each vector has a unique preimage. This inverse map is linear: if Mtx=u and Mty=v, then Mt(ax+by)=au+bv, so uniqueness identifies the inverse of au+bv with ax+by. Therefore Mt is invertible for every real t.

2.1F5F6step 1.1algebra

Put Nt=I+tK/2, so Mt∗=Nt. Since Mt and Nt are polynomials in K, they commute, and the same holds for Mt−1. For QK(t)=NtMt−1, the adjoint rules in [F5] give QK(t)∗=Nt−1Mt. Thus QK(t)∗QK(t)=Nt−1MtNtMt−1=I. In finite dimension this makes QK(t) unitary.

3.1F1F5F6step 2.1algebra

We have QK(0)=I. From M0′=−K/2 and [F5], (Mt−1)′∣t=0=K/2, hence the product rule gives QK′(0)=K. The curve PK(t)=QK(t)PQK(t)∗ lies in Pr: unitarity preserves self-adjointness and idempotence, and tr⁡(QK(t)PQK(t)∗)=tr⁡(PQK(t)∗QK(t))=tr⁡P by the finite trace identity tr⁡(AB)=tr⁡(BA). Its derivative at zero is PK′(0)=KP−PK=[K,P], so every such commutator is tangent.

4.1F2F6algebra∎

Conversely, by [F2] any tangent at P has block form HX=(0X∗X0) in range⁡P⊕(range⁡P)⊥. Set KX=(0−X∗X0), which satisfies KX∗=−KX. With P=(I000), block multiplication gives [KX,P]=HX. Thus every tangent is a skew-Hermitian commutator direction, proving the equality.

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