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Finite-dimensional linear isometries satisfy the adjoint identity

Statement

Let H,K be finite-dimensional (have finite bases by Finite-dimensional vector space, and its dimension dim⁡FV; infinite-dimensional means having no finite basis) complex inner-product spaces and let V:H→K be a linear isometry. Then V†V=IH. If V is also surjective, then VV†=IK.

Facts & Assumptions

Given: Finite-dimensional complex inner-product spaces H,K and a linear isometry V:H→K.

[F2]

Jordan–von Neumann: a norm is induced by an inner product exactly when it satisfies the parallelogram law: for the first-argument-linear complex pairing, ⟨x,y⟩=14(∥x+y∥2−∥x−y∥2+i∥x+iy∥2−i∥x−iy∥2).

[F3]

The adjoint T∗:W→V is characterised by ⟨Tv,w⟩W=⟨v,T∗w⟩V: the adjoint satisfies ⟨Vx,y⟩K=⟨x,V†y⟩H.

[F4]

Every linear map between finite-dimensional inner product spaces has a unique adjoint: every linear map between these finite-dimensional inner-product spaces has a unique adjoint.

Proof

1.1givenF1F2algebra

For all x,y∈H, [F2] expresses each inner product using the four displayed norm squares. Applying [F1] to x+y, x−y, x+iy, and x−iy therefore gives ⟨Vx,Vy⟩K=⟨x,y⟩H.

2.1givenF3F4F5step 1.1algebra

The adjoint exists by [F4]. By [F3] and step 1.1, ⟨x,(V†V−IH)y⟩H=0 for every x,y∈H. For each fixed y, conjugate symmetry and [F5] force (V†V−IH)y=0, hence V†V=IH.

3.1givenstep 2.1choosealgebra∎

If V is surjective, choose for arbitrary z∈K a vector x∈H with Vx=z. Step 2.1 gives VV†z=VV†Vx=Vx=z, so VV†=IK. The proof includes zero-dimensional spaces and uses only pointwise preimages, not a choice axiom.

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Sources