In quantum mechanics (QM), not all operators are Hermitian; only self-adjoint operators are. Anti-Hermitian operators, such as i times any Hermitian operator, exist and highlight this distinction. Observables must be represented by Hermitian operators to ensure real eigenvalues, which are essential for physical interpretation, such as energy values in the case of the Hamiltonian. The reality of eigenvalues is supported by the mathematical properties of Hermitian operators, which are derived from QM postulates. Ultimately, the choice of Hermitian operators allows for consistent physical outcomes regardless of the basis used in quantum state representation.