Alrahili Mazen, Savchuk Viktoriia, McNear Kelly, Pinchuk Anatoliy
Department of Physics and Energy Science, University of Colorado Colorado Springs, 1420 Austin Bluffs Parkway, Colorado Springs, CO, 80918, USA.
Physics Department, School of Science, Taibah University, Janadah Bin Umayyah Road, Medina, 42353, Saudi Arabia.
Sci Rep. 2020 Nov 2;10(1):18790. doi: 10.1038/s41598-020-75895-9.
We present a method for measuring the optical absorption cross section ([Formula: see text]) of gold nanoparticles (GNPs) based on optically heating the solution of GNPs with an 808 nm near-infrared (NIR) laser and measuring the temperature increase of the solution. We rely on the theoretical calculations based on the heat diffusion equations and experimental measurements based on the energy balance equations to measure the [Formula: see text] and the temperature distribution of single GNPs. Several morphologies, including gold nanospheres (GNSs), spherical gold nanoparticle conjugate (AuNPC), which are 20 nm GNSs surface-functionalized with an IR 808 dye, gold nanorods (GNRs), and gold nanourchins (GNUs), were studied. The study found that a single 20 nm GNS has the lowest [Formula: see text] and temperature distribution as compared to 100 nm GNUs. By increasing the size of GNSs from 20 to 30 nm, the magnitude of [Formula: see text] as well as temperature distribution increases by a factor of 5. The [Formula: see text] values of 20 and 30 nm GNSs calculated by Mie theory and the experimentally measured are in a good agreement. GNRs with equivalent radius ([Formula: see text]) 9.16 nm show the second lowest [Formula: see text]. By increasing the [Formula: see text] by a factor of 2 to 19.2 nm, the measured [Formula: see text] and temperature distribution also increased by a factor of 2. We also estimated [Formula: see text] for GNUs with diameters at 80 and 100 nm, which also have higher [Formula: see text] values. This work confirms that we can use temperature to accurately measure the [Formula: see text] of a variety of GNPs in solution.
我们提出了一种基于用808纳米近红外(NIR)激光对金纳米颗粒(GNP)溶液进行光学加热并测量溶液温度升高来测量金纳米颗粒光学吸收截面([公式:见正文])的方法。我们依靠基于热扩散方程的理论计算和基于能量平衡方程的实验测量来测量单个GNP的[公式:见正文]和温度分布。研究了几种形态,包括金纳米球(GNS)、球形金纳米颗粒共轭物(AuNPC,即表面用红外808染料功能化的20纳米GNS)、金纳米棒(GNR)和金纳米海胆(GNU)。研究发现,与100纳米GNU相比,单个20纳米GNS的[公式:见正文]和温度分布最低。将GNS的尺寸从20纳米增加到30纳米时,[公式:见正文]的大小以及温度分布增加了5倍。通过米氏理论计算的20纳米和30纳米GNS的[公式:见正文]值与实验测量值吻合良好。等效半径([公式:见正文])为9.16纳米的GNR的[公式:见正文]第二低。将[公式:见正文]增加2倍至19.2纳米时,测量的[公式:见正文]和温度分布也增加了2倍。我们还估计了直径为80纳米和100纳米的GNU的[公式:见正文],其[公式:见正文]值也更高。这项工作证实,我们可以利用温度准确测量溶液中各种GNP的[公式:见正文]。