Strong self-induced nonreciprocal transmission by using nonlinear PT-symmetric epsilon-near-zero metamaterials
Authors: Boyuan Jin, Christos Argyropoulos
AI-generated Key Points
- Investigate nonreciprocal transmission for unidirectional wave propagation
- Propose a compact and practical metamaterial based on SiC media separated by an air gap
- Photonically dope SiC media with gain and loss defects to achieve PT symmetry
- Exceptional point formed in the PT-symmetric system when SiC operates as ENZ material with moderate optical loss
- Strong self-induced nonreciprocal transmission excited due to nonlinear Kerr effect at slightly shifted frequency off the EP without breaking PT-symmetric phase
- Transmittance from one direction becomes unity while transmittance from other direction decreases to low values, allowing effective control of wave propagation
- Proposed active nonlinear metamaterial surpasses limitations of passive nonlinear nonreciprocal resonators enabling stronger nonreciprocity
- Enhancement of electric field in defects leads to extreme asymmetric field distribution upon excitation from opposite incident directions, contributing to strong self-induced nonreciprocal transmission and reducing required optical power
- Potential applications include developing nonreciprocal ultrathin coatings, circulators and isolators for controlling wave propagation.
Abstract: Nonreciprocal transmission is the fundamental process behind unidirectional wave propagation phenomena. In our work, a compact and practical parity-time (PT) symmetric metamaterial is designed based on two Silicon Carbide (SiC) media separated by an air gap and photonically doped with gain and loss defects. We demonstrate that an exceptional point (EP) is formed in this PT-symmetric system when SiC operates as a practical epsilon-near-zero (ENZ) material and by taking into account its moderate optical loss. Furthermore and even more importantly, strong self-induced nonreciprocal transmission is excited due to the nonlinear Kerr effect at a frequency slightly shifted off the EP but without breaking the PT-symmetric phase. The transmittance from one direction is exactly unity while the transmittance from the other direction is decreased to very low values, achieving very high optical isolation. The proposed active nonlinear metamaterial overcomes the fundamental physical bounds on nonreciprocity compared with a passive nonlinear nonreciprocal resonator. The strong self-induced nonreciprocal transmission arises from the extreme asymmetric field distribution achieved upon excitation from opposite incident directions. The significant enhancement of the electric field in the defects effectively decreases the required optical power to trigger the presented nonlinear response. This work can have a plethora of applications, such as nonreciprocal ultrathin coatings for the protection of sources or other sensitive equipment from external pulsed signals, circulators, and isolators.
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