Optical Waveguide Introduction Existing technology Much - PowerPoint PPT Presentation
Optical Waveguide Introduction Existing technology Much existing research has been done on silicon waveguides Optical fibre is an example of silicon waveguide technology Problem Transparency of silicon lies below 8m
Optical Waveguide
Introduction ● Existing technology ○ Much existing research has been done on silicon waveguides ○ Optical fibre is an example of silicon waveguide technology ● Problem Transparency of silicon lies below 8µm ○ Germanium with a transparency range of 1.6µm to 18µm is more suitable ○
Objective Determine the cut off dimensions of Single-mode Germanium on Silicon optical planar waveguide in mid-IR region
Total Internal Reflection ● For total internal reflection to occur, the propagating wave must be travelling in a medium of higher refractive index and hit a boundary with a lower refractive index . ● If angle of incidence > critical angle, total internal reflection will occur The critical angle can be derived by equating the angle of refraction to be 90. 𝑜 1 𝑡𝑗𝑜𝜄 𝑗 = 𝑜 2 𝑡𝑗𝑜𝜄 𝑠 𝑡𝑗𝑜𝜄 𝑗 = 𝑜 2 𝑡𝑗𝑜𝜄 𝑠 𝑜 1
Methodology ● Ran simulations with the software MODE Solutions by Lumerical
Parameters ● Wavelength of source: 3.8 µm Apart from the wavelength falling in the Mid-IR region, the actual laser source that is used in the lab now is a 3.8 µm laser. ● Germanium core ○ Transparency: 1.6 µm to 18 µm, suitable in the mid-IR region (2-20 µm). Refractive index of 4.03, higher than the silicon cladding with refractive ○ index of 3.42. Higher electron mobility at 3900 cm 2 V −1 s −1 compared to silicon’s ○ 1400 cm 2 V −1 s −1
Parameters ● Initial dimensions of germanium core: x span = 50 µm, y span = 2 µm, z span = 1.5 µm ○ ● Dimensions of substrate: ○ x span = 50 µm, y span = 50 µm, z span = 10 µm
Methodology ● Obtain the modal analysis for the first four modes. Modes 1&2 (TE 0 , TM 0 ) – Single Mode propagation ○ Modes 3&4 (TE 1 , TM 1 ) – Dual Mode propagation ○ ● Sweep the y and z span Obtain graph with y axis as effective refractive index and x axis as the y ○ span and z span in two separate graphs ● Determine the dimensions with the sweep results
Results
Results ● Modal analysis ● Ensure that first 2 modes are single mode, next 2 are dual Mode 1 Mode 2
Results Mode 3 Mode 4
Results ● Vary the y- and z-spans ● Obtain effective refractive index, neff , from the simulation ● Calculate cutoff dimension where neff > nSi
Results 3.42 Z-span Y-span
Results 3.42 3.42 Z-span
Results ● Cut-off dimensions obtained: 50µm by 2µm by 0.6µm ● Zhang.H. previously obtained values of 2 μ m and 1.38 μ m (y and z) ● Our results differ by 0.78 μ m in the z-span ● Accounts for Zhang’s high transmission loss ● Reduced loss
Conclusion
Conclusion ● Germanium has many applications in chemical sensing and environment monitoring ● We found out the cutoff dimensions for a single-mode Ge waveguide
Further Applications ● Detection of specific chemicals ● Optimising the waveguide dimensions to reduce loss
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