The all-ones matrix is diagonalizable for every . The vector together with the vectors from part (ii) is an eigenbasis. Independence follows because a multiple of has coordinate sum times that multiple, whereas every other basis vector has coordinate sum zero. In this basis the diagonal matrix is . At the one-vector basis suffices. Alternatively, the spectral theorem for real symmetric matrices applies. If dimension zero is allowed by the convention for , the empty matrix has no eigenvalues, an empty basis and a vacuous diagonalization.
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