We describe a novel modification of multimode-interference devices that has broad applicability. The modification involves introducing a slot (or slots), of a specific width and effective refractive index and at a specific position, that runs the longitudinal length of the multimode-interference region. Introducing N slots reduces the self-image length by a factor of N + 1. Varying the effective refractive index or width of the slot(s) creates a switch. The slot modification can be accomplished in a variety of ways, actually increases bandwidth, and has good error tolerances.
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http://dx.doi.org/10.1364/ao.43.006609 | DOI Listing |
Nanomaterials (Basel)
December 2024
State Key Laboratory of Integrated Optoelectronics, College of Electronic Science & Engineering, Jilin University, No. 2699 Qianjin Street, Changchun 130012, China.
A silica waveguide thermo-optic mode switch with small radius bimodal S-bends is demonstrated in this study. The cascaded multimode interference coupler is adopted to implement the E and E mode selective output. The beam propagation method is used in design optimization.
View Article and Find Full Text PDFNanophotonics
July 2024
State Key Laboratory of Precision Spectroscopy, East China Normal University, Shanghai 200062, China.
Polarization splitter-rotators (PSRs) are the key elements to realize on-chip polarization manipulation. Current PSRs on thin film lithium niobate (TFLN) rely on sub-micron gaps to realize mode separation, which increases the difficulties of lithography and etching. In this paper, a PSR on TFLN based on multimode interference (MMI) is demonstrated.
View Article and Find Full Text PDFNanomaterials (Basel)
September 2024
School of Energy and Power, Jiangsu University of Science and Technology, Zhenjiang 212003, China.
Based on the principle of self-imaging, a 1 × 2 graphene waveguide beam splitter is proposed in this work, which can split the graphene surface plasmons excited by far-infrared light. The multimode interference process in the graphene waveguide is analyzed by guided-mode propagation analysis (MPA), and then the imaging position is calculated. The simulation results show that the incident beam can be obviously divided into two parts by the self-imaging of the graphene surface plasmon.
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