Nony Laurent, Bocquet Franck, Loppacher Christian, Glatzel Thilo
Aix-Marseille Université, IM2NP, Centre Scientifique de Saint-Jérôme, Avenue Escadrille Normandie-Niemen, Case 151, F-13397 Marseille Cedex 20, France.
Nanotechnology. 2009 Jul 1;20(26):264014. doi: 10.1088/0957-4484/20/26/264014. Epub 2009 Jun 10.
The influence of short-range electrostatic forces on the measured local contact potential difference (CPD) by means of amplitude-modulation and frequency-modulation Kelvin probe force microscopy (AM- and FM-KPFM) is discussed on the base of numerical and analytical descriptions of both methods. The goal of this work is to help in interpreting recent experimental results reporting atomically resolved CPD images, in particular on bulk insulating samples. The discussion is carried out on the basis of spectroscopic curves. The expression of the bias-dependent electrostatic force is derived from a previous work and is estimated between a tip with simple geometry and the (001) facet of a perfect alkali halide single crystal. The force, with a short-range character, scales as a second-order polynomial function of the bias voltage. It is stated that the linear term is responsible for the occurrence of the atomic-scale CPD contrast, while the quadratic one, involving the sample polarization, accounts for the detected signal by the KPFM methods. Nevertheless, analytical and numerical approaches stress the influence of the linear term on the measured CPD which intrinsically hinders the possibility to perform quantitative CPD measurements, but also makes the measured 'pseudo-CPD' strongly deviating from the surface potential. Hence, in the short-range regime, AM- or FM-KPFM measurements neither reflect the CPD nor the local surface potential, but rather an effective value which is convoluted by the geometric parameters of the tip, the so-called local CPD. It is also stated that the local CPD measured by means of AM- or FM-KPFM differs when sub-nanometer vibration amplitudes of the cantilever are used. Otherwise, AM- and FM-KPFM measurements should be almost similar. At last, the influence of long-range, capacitive, electrostatic forces is discussed in conjunction with the short-range ones. This allows us to draw conclusions regarding the distance dependence of the local CPD which then exhibits a resonant behavior as a function of the tip-surface separation. This phenomenon is expected to play a role in the KPFM imaging process.
基于振幅调制和频率调制开尔文探针力显微镜(AM-KPFM和FM-KPFM)两种方法的数值和分析描述,讨论了短程静电力对测量的局部接触电势差(CPD)的影响。这项工作的目的是帮助解释最近报道的原子分辨CPD图像的实验结果,特别是在块状绝缘样品上的结果。讨论基于光谱曲线进行。偏置相关静电力的表达式源自先前的工作,并在具有简单几何形状的探针与完美碱金属卤化物单晶的(001)面之间进行了估算。该力具有短程特性,按偏置电压的二阶多项式函数缩放。据指出,线性项导致了原子尺度CPD对比度的出现,而涉及样品极化的二次项则解释了KPFM方法检测到的信号。然而,分析和数值方法强调了线性项对测量的CPD的影响,这本质上阻碍了进行定量CPD测量的可能性,但也使得测量的“伪CPD”与表面电势有很大偏差。因此,在短程范围内,AM-KPFM或FM-KPFM测量既不反映CPD也不反映局部表面电势,而是反映一个由探针几何参数卷积的有效值,即所谓的局部CPD。还指出,当使用亚纳米级悬臂振动幅度时,通过AM-KPFM或FM-KPFM测量的局部CPD会有所不同。否则,AM-KPFM和FM-KPFM测量应该几乎相似。最后,结合短程静电力讨论了长程电容性静电力的影响。这使我们能够得出关于局部CPD距离依赖性的结论,然后它表现为尖端与表面间距的函数的共振行为。预计这种现象在KPFM成像过程中会起作用。