Grobelny Jaroslaw, DelRio Frank W., Pradeep Namboodiri, Kim Doo-In, Hackley Vincent A., Cook Robert F.
Ceramics Division, Materials Science and Engineering Laboratory, National Institute of Standards and Technology
This assay protocol outlines the procedures for sample preparation of gold and the determination of nanoparticle size using atomic force microscopy (AFM). An AFM utilizes a cantilever with a sharp probe to scan a specimen surface. The cantilever beam is attached at one end to a piezoelectric displacement actuator controlled by the AFM. At the other end of the cantilever is the probe tip that interacts with the surface. At close proximity to the surface, the probe experiences a force (attractive or repulsive) due to surface interactions, which imposes a bending moment on the cantilever. In response to this moment, the cantilever deflects, and this deflection is measured using a laser beam that is reflected from a mirrored surface on the back side of the cantilever onto a split photodiode. A schematic diagram of the system is shown in Figure 1. The cantilever deflection is measured by the differential output (difference in responses of the upper and lower sections) of the split photodiode. The deflections are very small relative to the cantilever thickness and length. Thus, the probe displacement is linearly related to the deflection. The cantilever is typically silicon or silicon nitride with a tip radius of curvature on the order of nanometers. Based on the nature of the probe-surface interaction (attractive or repulsive), an AFM can be selected to operate in various modes, namely contact mode, intermittent contact mode, or non-contact mode. In contact mode, the interaction between the tip and surface is repulsive, and the tip literally contacts the surface. At the opposite extreme, the tip interacts with the surface via long-range surface force interactions; this is called non-contact mode. In intermittent contact mode, the cantilever is oscillated close to its resonance frequency perpendicular to the specimen surface, at separations closer to the sample than in non-contact mode. As the oscillating probe is brought into proximity with the surface, the probe-surface interactions vary from long range attraction to weak repulsion and, as a consequence, the amplitude (and phase) of the cantilever oscillation varies. During a typical imposed 100 nm amplitude oscillation, for a short duration of time, the tip extends into the repulsive region close to the surface, intermittently touching the surface and thereby reducing the amplitude. Intermittent contact mode has the advantage of being able to image soft surfaces or particles weakly adhered to a surface and is hence preferred for nanoparticle size measurements. A microscope feedback mechanism can be employed to maintain a user defined AFM set point amplitude, in the case of intermittent contact mode. When such feedback is operational, constant vibration amplitude can be maintained by displacing the built-in end of the cantilever up and down by means of the piezo-actuator. (Operation of an AFM with feedback off enables the interactions to be measured and this is known as force spectroscopy.) This displacement directly corresponds to the height of the sample. A topographic image of the surface can be generated by rastering the probe over the specimen surface and recording the displacement of the piezo-actuator as a function of position. Unlike electron microscopes, which provide a two-dimensional projection or a two-dimensional image of a sample, AFM provides a three-dimensional surface profile. Although the lateral dimensions are influenced by the shape of the probe, the height measurements can provide the height of nanoparticles with a high degree of accuracy and precision. If the particles are assumed to be spherical, the height measurement corresponds to the diameter or size of the particle. In this assay protocol, procedures for dispersing gold nanoparticles on various surfaces such that they are suitable for imaging and height measurement via intermittent contact mode AFM are first described. Generic procedures for AFM calibration and operation to make such measurements are then discussed. Finally, the procedures for data analysis and reporting are provided. The nanoparticles used to exemplify these procedures are National Institute of Standards and Technology (NIST) Au nanoparticle Reference Materials, RM 8011 (nominally 10 nm), RM 8012 (nominally 30 nm), and RM 8013 (nominally 60 nm), all of which contain citrate-stabilized negatively charged Au nanoparticles in an aqueous solution.
本检测方案概述了金的样品制备程序以及使用原子力显微镜(AFM)测定纳米颗粒尺寸的方法。AFM利用带有尖锐探针的悬臂扫描样品表面。悬臂梁的一端连接到由AFM控制的压电位移致动器上。悬臂的另一端是与表面相互作用的探针尖端。当靠近表面时,由于表面相互作用,探针会受到一个力(吸引力或排斥力),这会在悬臂上施加一个弯矩。作为对这个弯矩的响应,悬臂会发生偏转,并且使用从悬臂背面的镜面反射到分光光电二极管上的激光束来测量这种偏转。系统示意图如图1所示。悬臂的偏转通过分光光电二极管的差分输出(上下部分响应的差异)来测量。相对于悬臂的厚度和长度,偏转非常小。因此,探针位移与偏转呈线性关系。悬臂通常是硅或氮化硅材质,其尖端曲率半径在纳米量级。基于探针与表面相互作用的性质(吸引或排斥),可以选择AFM在各种模式下运行,即接触模式、间歇接触模式或非接触模式。在接触模式下,尖端与表面的相互作用是排斥性的,尖端实际上接触表面。在相反的极端情况下,尖端通过长程表面力相互作用与表面相互作用;这被称为非接触模式。在间歇接触模式下,悬臂在垂直于样品表面的方向上以接近其共振频率振荡,与样品的间距比非接触模式更近。当振荡的探针靠近表面时,探针与表面的相互作用从长程吸引力变为弱排斥力,结果,悬臂振荡的幅度(和相位)发生变化。在典型的施加100纳米幅度振荡过程中,在短时间内,尖端延伸到靠近表面的排斥区域,间歇性地接触表面,从而减小幅度。间歇接触模式的优点是能够对软表面或弱附着在表面的颗粒进行成像,因此在纳米颗粒尺寸测量中更受青睐。在间歇接触模式下,可以采用显微镜反馈机制来维持用户定义的AFM设定点幅度。当这种反馈运行时,可以通过压电致动器上下移动悬臂的内置端来维持恒定的振动幅度。(关闭反馈运行AFM能够测量相互作用,这被称为力谱学。)这种位移直接对应于样品的高度。通过在样品表面上扫描探针并记录压电致动器的位移作为位置的函数,可以生成表面的形貌图像。与提供样品二维投影或二维图像的电子显微镜不同,AFM提供三维表面轮廓。尽管横向尺寸受探针形状的影响,但高度测量可以高精度和高准确度地提供纳米颗粒的高度。如果假设颗粒是球形的,高度测量对应于颗粒的直径或尺寸。在本检测方案中,首先描述了将金纳米颗粒分散在各种表面上以便通过间歇接触模式AFM进行成像和高度测量的程序。然后讨论了进行此类测量的AFM校准和操作的通用程序。最后,提供了数据分析和报告的程序。用于举例说明这些程序的纳米颗粒是美国国家标准与技术研究院(NIST)的金纳米颗粒参考材料,RM 8011(标称10纳米)、RM 8012(标称30纳米)和RM 8013(标称60纳米),所有这些都在水溶液中含有柠檬酸盐稳定的带负电荷的金纳米颗粒。