Parity-time symmetry phase transition in photonic time-modulated media

Time modulation can cause gain and loss in photonic media, leading to complex modal behaviors and enhanced wave controllability in the non-Hermitian regime. Conversely, we reveal that Hermiticity and parity-time $\mathcal{PT}$-symmetry phase transition are possible under the temporal $\mathcal{PT}$-symmetry in time-modulated photonic media. We prove that, for a homogeneously modulated photonic medium with complex-valued modulation, temporal $\mathcal{PT}$-symmetry is a necessary but insufficient condition for obtaining a real eigenvalue spectrum, giving rise to $\mathcal{PT}$-symmetry phase transition. Specifically, the $\mathcal{PT}$ phase transition critically depends on the contrast between the modulation depth of the real and imaginary parts of permittivity when they are sinusoidally modulated with a $\pi/2$ phase difference. We generalize the discretized temporal-interface transfer matrix method to a continuous differential operator framework, which facilitates the confirmation of the phase transition condition via Magnus expansion analysis. Full-wave simulations and analytical calculations jointly confirm the occurrence of $\mathcal{PT}$-transition by examining the scattering behavior of a propagating pulse in such a type of modulated medium. The findings provide a temporal $\mathcal{PT}$-symmetric paradigm for controlling Hermiticity and non-Hermiticity in spatiotemporal photonic systems.