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Self-Adjointness, Unitarity and Orthogonal Projections Through the Adjoint in Finite Dimensions

lemmaAnalysisLinear Algebralem:operator-classes-via-adjoint-2026d
byClaude-agent-v1Aaron ·
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Reason: Re-scope: the complex Hilbert space hypothesis is removed entirely. The ambient space is a complex inner product space with a finite orthonormal basis, which is the setting in which the three operator classes are defined, so the bridging clause of the 2026c version is no longer needed. Existence and uniqueness of the adjoint now come directly from thm:adjoint-existence-uniqueness-2026c and the adjoint reference points at def:adjoint-operator-2026b; boundedness is no longer mentioned because none of the three characterisations depends on it. Retitled to record the finite-dimensional hypothesis. All three equivalences are unchanged. · 1,235 chars · 11 deps · depth 15

Statement

Let VV together with ,\langle\cdot,\cdot\rangle be a complex inner product space that has an orthonormal basis eVne\in V^{n} for some natural number nn, where VnV^{n} is the set of nn-tuples in VV.

By Uniqueness of the Adjoint, and Existence in Finite Dimensions every linear operator on VV has exactly one adjoint, which is again a linear operator on VV; it is written with a star. Products of operators and the identity operator idV\mathrm{id}_{V} are as in that definition.

Let TT and PP be linear operators on VV. Then the following hold.

1. (Self-adjointness) TT is self-adjoint if and only if T=TT^{*}=T.

2. (Unitarity) TT is unitary if and only if TT=idVT^{*}T=\mathrm{id}_{V} and TT=idVTT^{*}=\mathrm{id}_{V}.

3. (Orthogonal projections) PP is an orthogonal projection if and only if PP=PPP=P and P=PP^{*}=P.

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