Refractive Index*The refractive indices listed in this catalog were determined to the fifth decimal place for the following 20 lines of the spectrum. The refractive indices for dline (587.56 nm) and eline (546.07 nm) were determined to the sixth decimal place.
Table1
On the catalog pages, the wavelengths of each line are given in im units in parentheses under each spectrum line symbol. Dispersion*We have indicated (n_{F} n_{C}) and (n_{F´} n_{C´}) as the main dispersion. Abbe numbers were determined from the following νdand νe formula and calculated to the second decimal place:
ν_{d}=(n_{d}1)/(n_{F}n_{C}) ν_{e}=(n_{e}1)/(n_{F'}n_{C'})
We have also listed 12 partial dispersions (n_{x} n_{y} ), 8 relative partial dispersions for the main dispersion (n_{F} n_{C}) and 4 for (n_{F´} n_{C´}). To make achromatization effective for more than two wavelengths, glasses which have favorable relationships between νd and the relative partial dispersion e x,y for the wavelengths x and y are required. These may be defined as follows:
Constants of Dispersion FormulaThe refractive indices for wavelengths other than those listed in this catalog can be computed from a dispersion formula. As a practical dispersion formula, we have adopted the use of the Sellmeier formula shown below.
n^{2}1={A_{1}λ^{2}/(λ^{2}B_{1})}+{A_{2}λ^{2}/(λ^{2}B_{2})}+{A_{3}λ^{2}/(λ^{2}B_{3})}
The constants A_{1}, A_{2}, A_{3}, B_{1}, B_{2}, B_{3} were computed by the method of least squares on the basis of refractive indices at standard wavelengths which were measured accurately from several melt samples. By using this formula, refractive indices for any wavelength between 365 and 2325nm can be calculated to have an accuracy of around ±5 ×10–6 . These constants A_{1}, A_{2}, A_{3}, B_{1}, B_{2}, B_{3} are listed on the left side of the individual catalog pages. However in some glass types, not all refractive indices in the standard spectral range are listed on the data sheet. In such cases, the applicable scope of this dispersion formula is limited to the scope where refractive indices are given. When calculating a respective refractive index, please bear in mind that each wavelength is expressed in μm units. Thermal coefficient of refractive indices* (dn/dT)
Refractive index is affected by changes in glass temperature. This can be ascertained through the temperature coefficient of refractive index. The temperature coefficient of refractive index is defined as dn/dT from the curve showing the relationship between glass temperature and refractive index. The temperature coefficient of refractive index (for light of a given wavelength) changes with wavelength and temperature .
dn/dT_{absolute}=dn/dT_{relative}+n ·(dn_{air}/dT)
dn air /dT is the temperature coefficient of refractive index of air listed in Table 2.
Table2
The refractive indices in Ultraviolet and the Infrared RangeThe refractive indices in the ultraviolet and the infrared can be measured down to 157 nm in the ultraviolet and up to 2,325.42 nm in the infrared. Internal Transmittance*
Most types of OHARA optical glass are transparent and colorless because they are made of very pure materials. However, some optical glasses show remarkable absorption of light near the ultraviolet spectral range. For certain glasses with extreme optical properties, such as high refractive index, absorption extends to the visible range. Coloring*
Coloring can be determined by measuring spectral transmission, including reflection losses with test pieces of 10 mm
in thickness. The wavelengths corresponding to 80% transmission and 5% transmission are indicated as 405/355 in
units of 5nm, after rounding off 2 and rounding up 3 or more and rounding off 7 and rounding up 8 or more. Internal Transmittance λ80/λ5As the simple indicator of the coloring, the wavelengths that the internal transmittance is 80% and 5% are given. CCI (Colour Contribution Index)ISO Colour Contribution Index (ISO/CCI): The color characteristic index calculated by the method prescribed in JIS B70971986.


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