Quantum nonlinear effect in a dissipatively coupled optomechanical system

A full -quantum approach is used to study the quantum nonlinear properties of a compound Michelson-Sagnac interferometer optomechanical system. By deriving the effective Hamiltonian, we find that the reduced system exhibits a Kerr nonlinear term with a complex coefficient, entirely induced by the dissipative and dispersive couplings. Unexpectedly, the nonlinearities resulting from the dissipative coupling possess non -Hermitian Hamiltonian -like properties preserving the quantum nature of the dispersive coupling beyond the traditional system dissipation. This protective mechanism allows the system to exhibit strong quantum nonlinear effects when the detuning (the compound cavity detuning increment c and the auxiliary cavity detuning increment e) and the tunneling coupling strength (J) of two cavities satisfy the relation J2 = increment c increment e. Moreover, the additive effects of dispersive and dissipative couplings can produce strong anti -bunching effects, which exist in both strong and weak coupling conditions. Our work may provide a new way to study and produce strong quantum nonlinear effects in dissipatively coupled optomechanical systems.