• Journal of the European Optical Society-Rapid Publications
  • Vol. 20, Issue 1, 2024036 (2024)
Amit Halder*, Yeasin Arafat, Imtiage Ahmed, Muhammad Ahsan..., Zubairia Siddiquee, Riyad Tanshen and Shamim Anower|Show fewer author(s)
DOI: 10.1051/jeos/2024036 Cite this Article
Amit Halder, Yeasin Arafat, Imtiage Ahmed, Muhammad Ahsan, Zubairia Siddiquee, Riyad Tanshen, Shamim Anower. FEM analysis of a highly birefringent modified slotted core circular PCF for endlessly single mode operation across E to L telecom bands[J]. Journal of the European Optical Society-Rapid Publications, 2024, 20(1): 2024036 Copy Citation Text show less
Cross sectional view of proposed MSCCPCF. Where, Λ = 0.9 μm, d1/Λ = d2/Λ = d4/Λ = 0.45, d3/Λ = d6/Λ = 0.7, d5/Λ = 0.6 and d7/Λ = 0.85. Rectangular slot dimensions: a = Λ/2 and b = Λ/2√3.
Fig. 1. Cross sectional view of proposed MSCCPCF. Where, Λ = 0.9 μm, d1/Λ = d2/Λ = d4/Λ = 0.45, d3/Λ = d6/Λ = 0.7, d5/Λ = 0.6 and d7/Λ = 0.85. Rectangular slot dimensions: a = Λ/2 and b = Λ/2√3.
Quarter transverse cross-sectional view of air hole arrangement technique.
Fig. 2. Quarter transverse cross-sectional view of air hole arrangement technique.
Wavelength vs. effective refractive index curve.
Fig. 3. Wavelength vs. effective refractive index curve.
Wavelength-dependent dispersion characteristics of the proposed MSCCPCF.
Fig. 4. Wavelength-dependent dispersion characteristics of the proposed MSCCPCF.
Dispersion changes in response to a ± 1% variation in the pitch parameter of the MSCCPCF for (a) x-polarization and (b) y-polarization.
Fig. 5. Dispersion changes in response to a ± 1% variation in the pitch parameter of the MSCCPCF for (a) x-polarization and (b) y-polarization.
Dispersion changes in response to a ± 1% variation in the d1 to d7 diameter of the MSCCPCF for (a) x-polarization and (b) y-polarization.
Fig. 6. Dispersion changes in response to a ± 1% variation in the d1 to d7 diameter of the MSCCPCF for (a) x-polarization and (b) y-polarization.
Wavelength-dependent birefringence plot of the optimized MSCCPCF parameters.
Fig. 7. Wavelength-dependent birefringence plot of the optimized MSCCPCF parameters.
Variation of birefringence with (a) ±1% pitch adjustment and (b) ±1% variation of d1 to d7 in the proposed MSCCPCF.
Fig. 8. Variation of birefringence with (a) ±1% pitch adjustment and (b) ±1% variation of d1 to d7 in the proposed MSCCPCF.
Depiction of the wavelength-dependent relationship between effective area and nonlinear coefficient in the proposed MSCCPCF structure.
Fig. 9. Depiction of the wavelength-dependent relationship between effective area and nonlinear coefficient in the proposed MSCCPCF structure.
Plot demonstrating the wavelength-dependent numerical aperture of the proposed MSCCPCF.
Fig. 10. Plot demonstrating the wavelength-dependent numerical aperture of the proposed MSCCPCF.
Plot depicting the relationship between wavelength and confinement loss in the proposed MSCCPCF.
Fig. 11. Plot depicting the relationship between wavelength and confinement loss in the proposed MSCCPCF.
Plot illustrating the relationship between wavelength and confinement loss, demonstrating the impact of ±1% variation in (a) pitch value and (b) air hole diameters from d1 to d7 on the proposed MSCCPCF.
Fig. 12. Plot illustrating the relationship between wavelength and confinement loss, demonstrating the impact of ±1% variation in (a) pitch value and (b) air hole diameters from d1 to d7 on the proposed MSCCPCF.
Plot illustrating the wavelength-dependent variation of the V-number for the proposed MSCCPCF.
Fig. 13. Plot illustrating the wavelength-dependent variation of the V-number for the proposed MSCCPCF.
Wavelength dependent beat length plot of proposed MSCCPCF for optimum parameters.
Fig. 14. Wavelength dependent beat length plot of proposed MSCCPCF for optimum parameters.
Electromagnetic field distribution in the proposed MSCCPCF for (a) x-polarization, LP01x and (b) y-polarization, LP01y mode.
Fig. 15. Electromagnetic field distribution in the proposed MSCCPCF for (a) x-polarization, LP01x and (b) y-polarization, LP01y mode.
Ref./yearMaterials usedBirefringence, BNonlinear Coefficient, γ (W−1 km−1)Effective Area, Aeff (μm2)Confinement loss, αCL (dB/cm)Beat length, Lb [m]
[16]/2016Silica base3.373 × 10−22.2751.156 × 10−4
[17]/2017Silica base3.34 × 10−263.512.06910−9
[18]/2016Silica base3.474 × 10−238.372.656.359 × 10−4
[19]/2018Tellurite core and Slica base7.57 × 10−2188.39 2.98 × 10−112.047 × 10−5
[20]/2019Silica base12.046 × 10−361.471.71
[21]/2020Silica base3.76 × 10−250.342.3273.756 × 10−12 
[22]/2020Silica base3.85 × 10−250
[23]/2021Polytherimide (PEI) polymer base4.9 × 10−27.89 × 10−1131.61 × 10−6
[24]/2021Tellurite base5.05 × 10−218961.26
[25]/2022Tellurite base3.79 × 10−21672.361.4310−7
[26]/2023Silica base1.5 × 10−31.04 × 10−3
[27]/2023Silica base2.372 × 10−250.742.3973.07 × 10−8
[28]/2023Silica base3.56 × 10−216.719.43 × 10−8
[29]/2024Silica base3.5 × 10−315.647.4562.8 × 10−70.4483 × 10−3
Proposed MSCCPCFSilica base8.795 × 10−221.765.0855.615 × 10−1117.62 × 10−6
Table 1. Comparative assessment of optical characteristics at λ = 1.55 μm for proposed and prior PCFs.
Amit Halder, Yeasin Arafat, Imtiage Ahmed, Muhammad Ahsan, Zubairia Siddiquee, Riyad Tanshen, Shamim Anower. FEM analysis of a highly birefringent modified slotted core circular PCF for endlessly single mode operation across E to L telecom bands[J]. Journal of the European Optical Society-Rapid Publications, 2024, 20(1): 2024036
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