Author Affiliations
School of Materials Science and Engineering, Changchun University of Science and Technology, Changchun, Jilin 130022, Chinashow less
Fig. 1. Transverse cross section of the proposed MF
Fig. 2. Refractive index of bismuthate glasses and the effective index of x-polarized and y-polarized fundamental mode varying with wavelength (Λout=1.5 μm,dout/Λout=0.68,din/Λin=0.86)
Fig. 3. Electric field distribution of fundamental mode of MF at 3000-nm wavelength(Λout=1.5 μm,dout/Λout=0.68,din/Λin=0.86). (a) x-polarized; (b) y-polarized
Fig. 4. Influence of Λout on the dispersion and birefringence characteristics of MF when dout/Λout=0.68, din/Λin=0.86, Λout/Λin=3. (a) Dispersion of y-polarized fundamental mode; (b) dispersion of x-polarized fundamental mode; (c) birefringence of MF
Fig. 5. Influence of Λout on the effective mode field area of MF when dout/Λout=0.68, din/Λin=0.86,Λout/Λin=3. (a) y-polarized fundamental mode; (b) x-polarized fundamental mode
Fig. 6. Influence of dout/Λout on the dispersion and birefringence characteristics of MF when Λout=1.5 μm,din/Λin=0.86,Λout/Λin=3. (a) Dispersion of y-polarized fundamental mode; (b) dispersion of x-polarized fundamental mode; (c) birefringence of MF
Fig. 7. Influence of dout/Λout on the effective mode field area of MF when Λout=1.5 μm,din/Λin=0.86,Λout/Λin=3. (a) y-polarized fundamental mode; (b) x-polarized fundamental mode
Fig. 8. Influence of din/Λin on the dispersion and birefringence characteristics of MF when Λout=1.5 μm,dout/Λout=0.68,Λout/Λin=3. (a) Dispersion of y-polarized fundamental mode; (b) dispersion of x-polarized fundamental mode; (c) birefringence of MF
Fig. 9. Influence of din/Λin on the effective mode field area of MF when Λout=1.5 μm,dout/Λout=0.68,Λout/Λin=3. (a) y-polarized fundamental mode; (b) x-polarized fundamental mode