Let . This operator is self-adjoint, and
If condition (iii) holds, this quadratic form vanishes. For a real inner product, polarization gives
Therefore , which is condition (i). This supplies the nontrivial reverse implication needed for the equivalence.
By the definition of the adjoint,
If (i) holds, the expression is zero for all , giving (ii). Conversely, if this expression vanishes for every , nondegeneracy of the inner product gives for every , so (ii) also implies (i).
Taking in (ii) gives (iii). Together with (iii)(i) from part (i) and (i)(ii) from part (ii), this completes

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