Observation of parity-time symmetry breaking transitions in a dissipative Floquet system of ultracold atoms

Abstract

Open physical systems with balanced loss and gain, described by non-Hermitian parity-time ($\mathcal{P}\mathcal{T}$) reflection symmetric Hamiltonians, exhibit a transition which could engenders modes that exponentially decay or grow with time and thus spontaneously breaks the $\mathcal{P}\mathcal{T}$-symmetry. Such $\mathcal{P}\mathcal{T}$-symmetry breaking transitions have attracted many interests because of their extraordinary behaviors and functionalities absent in closed systems. Here we report on the observation of $\mathcal{P}\mathcal{T}$-symmetry breaking transitions by engineering time-periodic dissipation and coupling, which are realized through state-dependent atom loss in an optical dipole trap of ultracold ${}^6$Li atoms. Comparing with a single transition appearing for static dissipation, the time-periodic counterpart undergoes $\mathcal{P}\mathcal{T}$-symmetry breaking and restoring transitions at vanishingly small dissipation strength in both single and multiphoton transition domains, revealing rich phase structures associated to a Floquet open system. The results enable ultracold atoms to be a versatile tool for studying $\mathcal{P}\mathcal{T}$-symmetric quantum systems.

23 pages, 4 figures, 39 references