WebDec 28, 2024 · Optical nonreciprocity is an essential concept in optical signal processing and communication. The traditional way to achieve nonreciprocity is using magneto-optical nonreciprocal polarization rotation, which is incompatible with existing on-chip integration due to the applied magnetic field. Here, we theoretically and experimentally realize ... WebMar 31, 2024 · Controlling higher-order quantum nonreciprocity by spinning an optical resonator. We study how to achieve, manipulate, and switch classical or quantum nonreciprocal effects of light with a spinning Kerr resonator. In particular, we show that even when there is no classical nonreciprocity (i.e., with the same mean number of photons for …
Magnetic-free unidirectional polarization rotation and free-space ...
WebThe results provide compelling evidence for strong and tunable inelastic scattering effects under the triple resonance condition, fulfilled for optical transitions between neighboring high-Q lattice modes of the appropriate symmetry, which originate from multipolar Mie resonances. A consistent interpretation of the underlying mechanisms is ... WebJun 2, 2024 · The principle of magneto-optical nonreciprocity is to utilize the biasing static magnetic field to influence the electron cyclotron orbiting motion inside the material, which nonreciprocally affects electromagnetic wave propagation through the material. fly from southend to corfu
[2210.07038] Self-induced optical non-reciprocity
WebJul 14, 2024 · Nonreciprocal optical devices are important in wide areas, ranging from optical telecommunications to signal processing. Here, we experimentally realize the … WebJul 7, 2024 · This optical nonreciprocity response results from the constructive or destruction interference between different transmission paths in this multimode optomechanical system. We also show that the optical nonreciprocity response can be adjusted by the cavity decay rate, Coulomb coupling strength, intercavity tunneling strength. WebThe geometric dimensions of the designed thermal emitter for B = 1.5 T and angle of θ = 1° are: d = 7.53 μm, h g = 7.18 μm, f = 0.749, h = 3.3 μm. The corresponding spectral absorptivity, emissivity and the spectral nonreciprocity for B = 1.5 T and θ = 1° are calculated and plotted in Fig. 2 (a). Obviously, only one resonant emission peak and two very small … fly from southampton to manchester