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Numerical and experimental investigations of dependence of photoacoustic signals from gold nanoparticles on the optical properties

机译:从金纳米粒子对光学性质的光声信号依赖性的数值和实验研究

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摘要

Gold nanoparticles (AuNPs) are used as a contrast agent of the photoacoustic (PA) imaging. The efficiency of AuNPs has been discussed with the absorption cross section. However, the effects of the scattering of the light by AuNPs and surrounding medium on the PA signal from AuNPs have not been discussed. The PA signals from the aqueous solution of AuNPs were examined in the numerical simulation and the experiment. In the numerical simulation, the absorption and scattering cross sections of spherical and polyhedral AuNPs were calculated by Mie theory and discrete dipole approximation. Monte Carlo simulation calculated the absorbed light energy in the aqueous solution of AuNPs. Based on the PA wave equation, the PA signals were simulated. In the experiment, the PA signal from the aqueous solution of AuNP was measured by use of a piezoelectric film and a Q-switched Nd:YAG laser operated at 532 nm. The results of the numerical simulation and the experiment agreed well. In the numerical simulation and the experiment, a single Au nanocube with 50-nm edge generated the peak value of the PA signal significantly. It was approximately 350 times and twice as large as the peak values of the spherical AuNPs with 10- and 50-nm diameters, respectively. The peak value of the PA signal depended on both the absorption and scattering coefficients of the AuNPs and the surrounding medium. The peak value increased with the scattering coefficient in a quadratic manner. The character of the temporal profile of the PA signal such as full width at half maximum depended on the scattering coefficient of the AuNPs.
机译:金纳米颗粒(AUNP)用作光声(PA)成像的造影剂。已经用吸收横截面讨论了AUNP的效率。然而,尚未讨论从AUNP和周围介质对来自AUNPS的PA信号散射光的效果。在数值模拟和实验中检查来自剖砖水溶液的PA信号。在数值模拟中,通过MIE理论和离散偶极近似来计算球形和多面体AUNP的吸收和散射横截面。 Monte Carlo仿真计算了AuNP水溶液中的吸收光能。基于PA波动方程,模拟了PA信号。在实验中,通过使用压电膜和Q开关Nd:在532nm处操作的Q开关Nd:Q开关Nd:Q开关Nd:Q开关Nd:Q开关的Nd:Q开关Nd:Q开关Nd:Q开关的Nd:在532nm处进行测量的PA信号。数值模拟的结果和实验吻合良好。在数值模拟和实验中,具有50nm边缘的单个Au纳米轴,显着产生了PA信号的峰值。它分别大约350次,分别是球形AUNP的峰值分别具有10-和50nm直径的两倍。 PA信号的峰值取决于AUNP和周围介质的吸收和散射系数。峰值以二次方式随着散射系数而增加。 PA信号的时间轮廓的特征,例如半宽度的全宽度依赖于AUNP的散射系数。

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