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Nyström is a square-root orthogonal-projection compression

Statement

Let F∈{R,C}, n≥1, s≥0, A∈Fn×n be Hermitian positive semidefinite, S∈Fn×s, and B=A1/2S. If PRan⁡(B) denotes the orthogonal projection onto the range of B, then

A^nys=A1/2PRan⁡(B)A1/2=A1/2B(B∗B)†B∗A1/2=A1/2BB†A1/2.

Facts & Assumptions

Given: A finite Hermitian positive-semidefinite matrix A, a sketch S, and B=A1/2S.

[F1]

The positive-semidefinite Nyström approximation: A^nys=AS(S∗AS)†S∗A.

[F2]

The Moore-Penrose products are orthogonal projectors: for any finite B, BB† and B†B are orthogonal projections onto Ran⁡(B) and Ran⁡(B†).

[F3]

Every finite real or complex matrix has a unique Moore--Penrose pseudoinverse: every finite matrix has a unique Moore-Penrose inverse.

[F4]

A non-negative operator has a unique non-negative square root: A has a unique Hermitian positive-semidefinite square root A1/2 satisfying (A1/2)2=A.

[F5]

The Moore--Penrose pseudoinverse A+ as the solution of the four Penrose equations: a Moore-Penrose inverse is specified by the four Penrose equations.

Proof

1.1F1F4algebra

Set D=B∗B=S∗AS. From (A1/2)2=A and A1/2=(A1/2)∗, [F1] rewrites as A^nys=A1/2BD†B∗A1/2.

1.2F3F5algebra

Since D=D∗, taking adjoints of the four defining equations [F5] shows (D†)∗ also satisfies them for D. Uniqueness [F3] gives (D†)∗=D†. Thus P=BD†B∗ is self-adjoint, and P2=BD†(B∗B)D†B∗=BD†DD†B∗=P by the Moore-Penrose equation D†DD†=D†. Hence P is an orthogonal projection.

1.3F2F3F5algebra

Put Q=D†D. By [F2], Q is an orthogonal projection. The equations [F5] DD†D=D and D†DD†=D† imply DQ=D; therefore Qx=0 iff Dx=0. Also x∗Dx=∥Bx∥22, so ker⁡D=ker⁡B. Since Q is an orthogonal projection, Ran⁡(I−Q)=ker⁡Q=ker⁡B, and consequently B(I−Q)=0, or BQ=B.

2.1F2step 1.1step 1.3algebra∎

Step 1.3 gives PB=BD†D=BQ=B. Since P has range contained in Ran⁡(B) and fixes every vector in Ran⁡(B), its range is exactly Ran⁡(B). Thus P=PRan⁡(B). The projector BB† has the same range by [F2]. For each vector, orthogonal projection decomposes it uniquely into a component in Ran⁡(B) and one in its orthogonal complement, so these two projectors coincide. Substituting this identity into step 1.1 proves all displayed formulas.

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