Laser & Optoelectronics Progress, Volume. 60, Issue 17, 1723001(2023)

Polarization-Independent Optical Power Splitter with a Designable Splitting Ratio

Jingli Wang1、*, Haiguang Liu1, Yueteng Zhang1, Yuchen Song1, Hanxiao Shen1, Heming Chen2, and Kai Zhong3
Author Affiliations
  • 1College of Electronic and Optical Engineering & College of Flexible Electronics (Future Technology), Nanjing University of Posts and Telecommunications, Nanjing 210023, Jiangsu , China
  • 2Bell Honors School, Nanjing University of Posts and Telecommunications, Nanjing 210023, Jiangsu , China
  • 3Key Laboratory of Optoelectronics Information Technology (Ministry of Education), School of Precision Instruments and Opto-Electronics Engineering, Tianjin University, Tianjin 300072, Jiangsu , China
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    Figures & Tables(11)
    Structure diagram of the polarization-independent optical power splitter with designable splitting ratio. Inset: section view of the sandwich structure
    fIL as functions of L
    Field distribution in the sandwich structures. (a) TE polarization mode; (b) TM polarization mode
    nSiNx corresponding to TE and TM polarization modesas a function of nSiNx, when g1=140 nm
    nSiNx as a function of g1 when polarization-independent condition is satisfied
    Polarization-independent condition is satisfied. (a) fSR as a function of g1; (b) fILas a function of g1
    Field distribution of devices with different Pout1∶Pout2. (a) 50∶50, TE; (b) 50∶50, TM; (c) 40∶60, TE; (d) 40∶60, TM; (e) 30∶70, TE; (f) 30∶70, TM; (g) 20∶80, TE; (h) 20∶80, TM; (i) 10∶90, TE; (j) 10∶90, TM
    ΔfSR¯ and fIL¯ as functions of Ws and Ls. (a)30:70, ΔfSR¯; (b) 30:70, fIL¯; (c) 10:90, ΔfSR¯; (d)10:90, fIL¯
    fSR and fIL as a function of wavelength when the Pout1∶Pout2 of device are 50∶50, 40∶60, 30∶80, 20∶80 and 10∶90 respectively. (a) fSR; (b) fIL
    • Table 1. Parameters and performance of devices with different fSR when polarization-independent condition is satisfied

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      Table 1. Parameters and performance of devices with different fSR when polarization-independent condition is satisfied

      fSRPout1Pout2g1 /nmnSiNxfIL(TE)/dBfIL(TM)/dB
      0.550∶501003.200.040.02
      0.640∶601242.910.070.03
      0.730∶701532.680.090.03
      0.820∶801982.370.140.03
      0.910∶902732.030.260.10
    • Table 2. Comparison of performance of optical power splitters with designable fSR

      View table

      Table 2. Comparison of performance of optical power splitters with designable fSR

      ReferenceStructureSizeRange of fSRBandwidth /nmfIL /dBPolarization
      11MMI3.6 μm×3.6 μm0.50‒0.80300.97dependent
      14Y-junction1.4 μm×2.3 μm0.50‒0.981000.36dependent
      15AC4 μm×240 μm0.50‒0.931001.00dependent
      16ACL=80 μm0.50‒1.001000.05dependent
      13DCL<30 μm0.50‒1.00

      100

      fSR=0.50)

      0.10

      fSR=0.50)

      independent
      Our workSandwich ACL=7 μm0.50‒0.951000.31(0.17)independent
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    Jingli Wang, Haiguang Liu, Yueteng Zhang, Yuchen Song, Hanxiao Shen, Heming Chen, Kai Zhong. Polarization-Independent Optical Power Splitter with a Designable Splitting Ratio[J]. Laser & Optoelectronics Progress, 2023, 60(17): 1723001

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    Paper Information

    Category: Optical Devices

    Received: Jul. 3, 2022

    Accepted: Sep. 13, 2022

    Published Online: Sep. 13, 2023

    The Author Email: Jingli Wang (jlwang@njupt.edu.cn)

    DOI:10.3788/LOP222232

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