A density matrix has unit trace. The Pauli matrices are traceless, so and hence . Using in the expectation value gives
Consequently the required Bloch vector and density matrix are
The two eigenvalues are and , both positive, so this is a valid density operator. Its purity of a density operator is
Therefore it is a mixed state. Equivalently, its spectral decomposition is , an ensemble of the two distinct spin one-half along an axis states, rather than a single pure state.

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