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BaF2-GdF3-ZrF4-AlF3玻璃的折射率色散

Refractive-index dispersion for BaF2-GdF3-ZrF4-AlF3 glasses.

作者信息

Mitachi S, Miyashita T

机构信息

NTT Ibaraki Electrical Communication Laboratory, Tokai, Ibaraki-ken 319-11, Japan.

出版信息

Appl Opt. 1983 Aug 15;22(16):2419-25. doi: 10.1364/ao.22.002419.

Abstract

Refractive-index dispersion measurements were performed on bulk specimens of 2-, 4-, or 6-mol % AlF(3) doped 33BaF(2)-4GdF(3)-63ZrF(4) (mol %) glass and 4-mol % LiF, CsF, YF(3), CdF(2), SnF(2), or PbF(2) doped 31.68BaF(2)-3.84GdF(3)-60.48ZrF(4)-4AIF(3) (mol %) glass in the wavelength region from 0.4047 to 5.3036 microm. The material dispersion curve and zero material dispersion wavelength were estimated on the basis of refractive- index dispersion measurements. The slope of the material dispersion curve for these fluoride glasses was less steep than that for SiO2 glass in the wavelength range estimated. The zero material wavelength lambda(0) shifted to a shorter wavelength with increasing AlF3 concentration. The lambda(0) is 1.675 microm for 31.68BaF(2)- 3.84GdF(3)-60.48ZrF(4)-4AlF(3) (mol %) glass. When 4-mol % LiF, CsF, YF(3), CdF(2), SnF(2), or PbF(2) were doped into these glasses, each lambda(0) shifted from 1.675 to 1.670, 1.668, 1.673, 1.681, 1.683, or 1.704 microm, respectively. The temperature dependence values of the refractive-index dispersion and material dispersion for 31.68BaF(2)-3.84GdF(3) -60.48ZrF(4)-4AIF(3) (mol %) glass were also obtained. The temperature coefficients of the refractive index were negative values (dn/dT(relative) = -1.0 X 10(-5)/degrees C) and the wavelength dependence of dn/dT was small. The wavelength lambda(0) shifted from 1.675 to 1.605 microm, due to the rise in the measurement temperature from 25 degrees C to 250 degrees C.

摘要

对2摩尔%、4摩尔%或6摩尔% AlF₃掺杂的33BaF₂ - 4GdF₃ - 63ZrF₄(摩尔%)玻璃以及4摩尔% LiF、CsF、YF₃、CdF₂、SnF₂或PbF₂掺杂的31.68BaF₂ - 3.84GdF₃ - 60.48ZrF₄ - 4AlF₃(摩尔%)玻璃的块状样品在0.4047至5.3036微米的波长范围内进行了折射率色散测量。基于折射率色散测量估算了材料色散曲线和零材料色散波长。在估算的波长范围内,这些氟化物玻璃的材料色散曲线斜率比SiO₂玻璃的斜率平缓。随着AlF₃浓度增加,零材料波长λ(0)移向更短波长。对于31.68BaF₂ - 3.84GdF₃ - 60.48ZrF₄ - 4AlF₃(摩尔%)玻璃,λ(0)为1.675微米。当向这些玻璃中掺杂4摩尔% LiF、CsF、YF₃、CdF₂、SnF₂或PbF₂时,每个λ(0)分别从1.675移至1.670、1.668、1.673、1.681、1.683或1.704微米。还获得了31.68BaF₂ - 3.84GdF₃ - 60.48ZrF₄ - 4AlF₃(摩尔%)玻璃的折射率色散和材料色散的温度依赖性值。折射率的温度系数为负值(dn/dT(相对) = -1.0×10⁻⁵/℃),且dn/dT的波长依赖性较小。由于测量温度从25℃升至250℃,波长λ(0)从1.675移至1.605微米。

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