An arbitrary operator A can be expressed as A = B + iC, where B and C are Hermitian operators. This is demonstrated by rewriting A using the formula A = (A + A†)/2 + (A - A†)/2. The first term, (A + A†)/2, is Hermitian, while the second term, (A - A†)/2, is anti-Hermitian, leading to the conclusion that A can be decomposed into Hermitian components. The discussion emphasizes that this decomposition holds true for any operator with an involution J, allowing for a similar representation. Understanding this relationship is fundamental in the study of Hermitian operators.