“…2. 1, 2, 3, and 4 are the different operating points of the broad-spectrum light source-driven RFOG, and I1, I2, I3, and I4 are the light intensities at the corresponding operating points, which are defined similarly to that of the IFOG [6][7] .The traditional modulation scheme of the broad-spectrum light source-driven RFOG is to modulate the system by the frequency shifting function of the MIOC at the operating points 1 and 2. modulation of the system. In the open-loop state, after the working point is determined, the optical power-frequency conversion coefficient k is also determined, so the light intensity change can be considered to be approximately linear, and at this time the angular velocity Ω can be expressed as:…”