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基于Tikhonov反演的退偏振动态光散射法棒状颗粒测量

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利用退偏振动态光散射法测量棒状纳米颗粒尺寸时,计算过程中通常使用指数拟合算法,但该算法受初始值的影响较大,选取的初值不同拟合结果也不同。为解决该问题,提出利用Tikhonov正则化算法对退偏振动态光散射实验获得的垂直偏振和水平偏振自相关函数进行反演,从而得到平移和旋转衰减线宽,再计算得出平移扩散系数和旋转扩散系数,进而拟合得到纳米棒的长度和直径。搭建了退偏振动态光散射实验装置,对三种金纳米棒样品进行了退偏振动态光散射测量。实验结果表明,经过修正去掉吸附层后,金纳米棒的长度和直径测量值与透射电子显微镜(TEM)测量值相比,其偏差在8%以内,这表明修正后的测量结果与TEM的测量结果一致性较好。
Depolarized Dynamic Light Scattering Method for Rod-Shaped Particle Measurement Based on Tikhonov Inversion
Objective The properties of nanoparticles are related to their structures and sizes,and studying methods for measuring the length and diameter of rod-shaped nanoparticles is of practical significance.Transmission electron microscopy has high resolution and can provide detailed morphological features of rod-shaped nanoparticles.However,electron microscopy can only observe a small number of particles,and the measurement results lack statistical significance.The dynamic light scattering method can quickly characterize the particle size and size distribution of nanoparticles,but since this method assumes that the measured particles are spherical,it cannot accurately measure the size of rod-shaped particles.The depolarization dynamic light scattering method can obtain the length and diameter of rod-shaped nanoparticles by measuring the translational and rotational diffusion coefficients of particles in Brownian motion.It is necessary to fit the translational and rotational attenuation linewidths separately for obtaining the translational and rotational diffusion coefficients of the Brownian motion of rod-shaped nanoparticles.Exponential fitting algorithms are commonly adopted in fitting the attenuation linewidth,but they are greatly affected by the initial value.When the initial value is not suitable,the measurement results will deviate from the true value.To this end,a Tikhonov regularization algorithm is proposed to invert the vertical and horizontal polarization autocorrelation functions obtained from depolarized dynamic light scattering experiments,thereby putting forward a method for acquiring the translational and rotational attenuation linewidths.Methods The experimental device employs a 532 nm vertically polarized solid-state laser as the light source,and a Glen Thompson lens is placed at a 90° scattering angle position.The lens divides the scattered light into two optical paths of horizontal polarization and vertical polarization.On each path,a single-mode fiber is utilized to receive the scattered light signal,which is then fed into a photomultiplier tube.After receiving the scattered light signal,the normalized autocorrelation function of light intensity is obtained by real-time calculation of a large dynamic range high-speed digital correlator.Additionally,the temperature control system maintains the sample cell temperature at 25℃.During the experiment,the experimental device is covered with a shell to prevent interference from stray light and reduce measurement errors.Three different sizes of gold nanorod samples are purchased,and four different concentrations of gold nanorod samples are set for depolarization dynamic light scattering measurements.The autocorrelation functions of vertical and horizontal polarization directions of samples with different concentrations are obtained.The Tikhonov regularization algorithm is adopted to invert the autocorrelation function to obtain the translational and rotational attenuation linewidths.After converting the attenuation linewidth into diffusion coefficient,the Tirado-Garcia de la Torre(TG)model can be leveraged to fit the length and diameter of rod-shaped nanoparticles.Since rod-shaped gold nanoparticles are surrounded by an adsorption layer in the liquid,the adsorption layer increases the size of the rod-shaped gold nanoparticles,making their size slightly larger than the actual size in the liquid.Therefore,we have corrected the three sets of length and diameter data obtained from depolarized dynamic light scattering measurements.The measurement results are compared with those of a transmission electron microscope to verify the feasibility of this method.Results and Discussions After Tikhonov regularization inversion of the horizontal polarization autocorrelation function,a single-peak attenuation linewidth distribution can be obtained,and the mixed attenuation linewidth can be obtained from its peak[Fig.7(a)].After performing Tikhonov regularization inversion on the vertical polarization autocorrelation function,a bimodal attenuation linewidth distribution is obtained,and the translational attenuation linewidth can be acquired from its left peak[Fig.7(b)].The original concentrations of the three samples are all 0.1 mg/ml,and samples with different concentrations of 0.10,0.07,0.05,and 0.03 mg/ml respectively are obtained by diluting them.The experimental data show that the autocorrelation functions of light intensity of samples with different concentrations coincide,with consistent measurement results(Fig.3).Conclusions We propose to employ the Tikhonov regularization algorithm to invert the autocorrelation functions in the horizontal and vertical polarization directions,respectively and thus to obtain the translational and rotational attenuation linewidths.After converting the attenuation linewidths into diffusion coefficients,the length and diameter of rod-shaped nanoparticles can be fitted using the TG model.The experimental results show that after removing the adsorption layer after correction,the length and diameter measurements of three sets of rod-shaped gold nanoparticles obtained using the depolarization dynamic light scattering method based on Tikhonov inversion are within 8%of the measurement results of transmission electron microscopy.This indicates that the corrected measurement results are consistent with the measurement results of transmission electron microscopy.The experimental data demonstrate that the autocorrelation functions of light intensity of samples with different concentrations basically coincide,and the measurement results remain consistent.

depolarized dynamic light scatteringgold nanorodtranslational diffusion coefficientrotational diffusion coefficientpolydispersity

尹秀文、刘伟、綦华宇、王雅静、秦福元

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山东理工大学电气与电子工程学院,山东 淄博,255049

澳谱特科技(上海)有限公司,上海,201109

退偏振动态光散射 金纳米棒 平移扩散系数 旋转扩散系数 多分散性

山东省自然科学基金

ZR2020MF124

2024

光学学报
中国光学学会 中国科学院上海光学精密机械研究所

光学学报

CSTPCD北大核心
影响因子:1.931
ISSN:0253-2239
年,卷(期):2024.44(4)
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