Fig. 2: Exceptional point in a gain-loss coupled cavity.
From: Dynamic gain and frequency comb formation in exceptional-point lasers

a A coupled 1D cavity separated by a distributed Bragg reflector (DBR), with gain in the left cavity and absorption in the right cavity. Gray-scale colors indicate the cold-cavity permittivity profile εc(x). Orange and blue shades show the gain and absorption profiles Dp(x) and σ(x), respectively. b, c The two relevant eigenvalues, \({\tilde{\omega }}_{0}\) and \({\tilde{\omega }}_{1}\), of the linear operator \(\hat{O}\left(\omega \right)\) in Eq. (4) with a linear gain D0(x) = Dp(x), as a function of the pumping strength \({D}_{\max }\) and the length of the passive cavity, L2 = 1340 nm + Δ. The two eigenvalues meet at an EP (green circle). The absorption in the passive cavity is σ/ε0 = 4.9 ps−1. The red and blue curves indicate \({\tilde{\omega }}_{0}\) and \({\tilde{\omega }}_{1}\) with Δ = 0. d Eigenvalue trajectories on the complex-frequency plane for Δ = 0, with the orange arrows indicating the directions of increasing \({D}_{\max }\). Open circles indicate \({D}_{\max }=0\), and filled red and blue circles indicate the first lasing threshold \({D}_{\max }={D}_{1}^{{{\rm{th}}}}\) where \({\tilde{\omega }}_{0}\) reaches the real-frequency axis. Dashed lines show the would-be above-threshold trajectories in the absence of gain saturation.