“…Previous works assumed the optical devices to be characterised by an all-phase transfer function [1][2][3], where the optical phase, was approximated by a finite order Taylor expansion around the optical centre frequency. However, present day optical devices have more complex transfer functions, including both phase and amplitude variations, at higher RF frequencies (millimetre waves) and with ever-wider RF bandwidths [4], requiring a more generalised matrix. This Letter derives such a matrix, valid for small signal modulation.…”