“…is the creation operator for the dark modes. 5 The bright mode part of the Hamiltonian (the first three terms of S12, without dark mode terms ๐บ U ๐ ) can be recognized as similar to Jaynes-Cumming model with gโGN, and ฯoโ๐บ U ๐ replacing, thereby has the same solutions as Jaynes-Cumming model but with replaced terms. Thus, the g value obtained from the fitting in the previous section, Harmonic oscillator fitting model, (with results in section 7) is equivalent to GN for the quartz-pillar resonator.…”