Since $A=B+iC$ with $B$ and $C$ hermitian, we can decompose the inner product thanks to the linearity in its second argument
$$
\langle \psi | A \psi \rangle=\langle \psi | (B \psi+iC \psi) \rangle=\langle \psi | B \psi \rangle+\langle \psi | iC \psi \rangle
$$
We can use the spectral decomposition: $B=Q^\dagger DQ$ and $C=Q'^\dagger D'Q'$ where $Q,Q'$ are orthogonal and $D,D'$ are diagonal matrices of real values.
$$
\langle \psi | B \psi \rangle+\langle \psi | iC \psi \rangle=
\langle \psi | Q^\dagger DQ \psi \rangle+\langle \psi | iQ'^\dagger D'Q' \psi \rangle
$$
Since the inner product is invariant with respect multiplication of orthogonal matrices
$$
\langle \psi | Q^\dagger DQ \psi \rangle+\langle \psi | iQ'^\dagger D'Q' \psi \rangle=
\langle \psi | D \psi \rangle+\langle \psi | iD' \psi \rangle
$$
If the $j$-th component of $|\psi\rangle$ is $(x_j+iy_j)$, the innero product $\langle \psi | D \psi \rangle$ can be written as
$$
b=\sum_j (x_j+iy_j)(x_j-iy_j)d_j=\sum_j (x_j^2+iy_j^2)d_j
$$
that is a real number.
Reasoning in a analogues way we have that $\langle \psi | iC \psi \rangle$ is a complex number, therefore it should be null.
We can conlcude that $A=B=Q^\dagger D Q$, i.e. $A$ is an hermitian operator.