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Measurement of Scattering and Absorption Cross Sections of Microspheres for Wavelengths between 240 nm and 800 nm

机译:在240 nm至800 nm波长范围内测量微球的散射和吸收截面

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摘要

A commercial spectrometer with a 150 mm integrating sphere (IS) detector was used to estimate the scattering and absorption cross sections of monodisperse polystyrene microspheres suspended in water. Absorbance measurements were performed with the sample placed inside the IS detector. The styrene absorption was non zero for wavelengths less than 300 nm. Correction for fluorescence emission by styrene was carried out and the imaginary part of the index of refraction, ni, was obtained. Absorbance measurements with the sample placed outside the IS detector were sensitive to the loss of photons from the incident beam due to scattering. The absorbance data was fitted with Lorenz-Mie scattering cross section and a correction for the finite acceptance aperture of the spectrometer. The fit parameters were the diameter, the suspension concentration, and the real part of the index of refraction. The real part of the index was parameterized using an expansion in terms of powers of the inverse wavelength. The fits were excellent from 300 nm to 800 nm. By including the imaginary part obtained from the absorbance measurements below 300 nm, it was possible to obtain a good fit to the observed absorbance data over the region 240 nm to 800 nm. The value of ni at 266 nm was about 0.0060±0.0016 for microspheres with diameters of 1.5 μm, 2.0 μm, and 3.0 μm. The scattering cross section, absorption cross section, and the quantum yield at 266 nm of microsphere with a diameter of 2.0 μm was 5.65±0.01 μm2, 1.54±0.03 μm2, and 0.027±0.002 respectively. The styrene absorption reduces the scattering cross section by 20 % at 266 nm.
机译:使用带有150毫米积分球(IS)检测器的商用光谱仪来估算悬浮在水中的单分散聚苯乙烯微球的散射和吸收截面。吸光度测量是将样品置于IS检测器内部进行的。对于小于300 nm的波长,苯乙烯吸收为非零。进行了苯乙烯的荧光发射的校正,并且获得了折射率的虚部ni。将样品置于IS检测器外部的吸光度测量对由于散射而导致的入射光束中光子的损失非常敏感。将吸光度数据与Lorenz-Mie散射截面和光谱仪的有限接收孔径进行校正。拟合参数是直径,悬浮液浓度和折射率的实部。使用反波长功率的扩展来参数化索引的实部。从300 nm到800 nm的拟合非常好。通过包含从低于300 nm的吸光度测量获得的虚部,可以很好地拟合240 nm至800 nm区域内观察到的吸光度数据。对于直径为1.5μm,2.0μm和3.0μm的微球,在266nm处的ni值约为0.0060±0.0016。直径为2.0μm的微球在266 nm处的散射截面,吸收截面和量子产率为5.65±0.01μm 2 ,1.54±0.03μm 2 ,分别为0.027±0.002。苯乙烯吸收在266 nm下将散射横截面减小了20%。

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