Explicit construction of Floquet–Bloch states from arbitrary solution bases of the Hill equation

Abstract For the Hill equation describing one-dimensional periodic systems, an explicit construction of Floquet–Bloch states from arbitrary pairs of linearly independent solutions is developed. Closed-form formulas map an arbitrary fundamental system to a Floquet–Bloch basis via the monodromy matrix, including the generic Jordan band-edge case, without reliance on canonically normalized solutions. An equivalent transfer-matrix formulation makes the residual representation freedom transparent and provides a practical framework for analytical and numerical studies of periodic systems.