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Noncontact Atomic Force Microscopy - Yale School of Engineering ...

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Short and medium range electrostatic forces analyzed by<br />

Kelvin probe force microscopy<br />

Th. Glatzel, S. Kawai, S. Koch, A. Barat<strong>of</strong>f, and E. Meyer<br />

Department <strong>of</strong> Physics, University <strong>of</strong> Basel, 4056 Basel, Switzerland.<br />

Tu-1510<br />

We discuss the influences <strong>of</strong> short and medium range electrostatic forces on the local<br />

contact potential difference (LCPD) by means <strong>of</strong> amplitude modulated Kelvin probe<br />

force microscopy (AM-KPFM) measured on single crystal KBr(100) surfaces. Bias- and<br />

z-spectroscopic curves at atomic scale showing clear features related to the influence <strong>of</strong><br />

the short range electrostatic interaction [1].<br />

In Fig.1 a typical nc-AFM /KPFM measurement <strong>of</strong> a KBr(100) in UHV is shown. While<br />

the topography (a) was measured at the first resonance frequency <strong>of</strong> the cantilever<br />

(approx 160kHz), the LCPD image (b) was measured by compensating the inphase signal<br />

detected at he second resonance (approx 1MHz). A clear contrast between the different<br />

ionic sides is observed. To clarify the origin <strong>of</strong> this contrast we performed bias- and zspectroscopy<br />

measurements. c) shows a bias-spectroscopy measurement illustrating the<br />

amplitude R, the inphase signal X, and the frequency shift at a maxima <strong>of</strong> the topography.<br />

Comparing these measurements with the ones at the minimas <strong>of</strong> the topography (not<br />

presented here) clearly shows the expected CPD difference.<br />

Figure 1: Typical topography (3x3nm 2 , �z=100pm) and<br />

local contact potential image (�LCPD=300mV) <strong>of</strong> a<br />

KBr(100) surface. In c) the lockin signals amplitude R,<br />

inphase X (second resonance <strong>of</strong> the cantilever) as well as<br />

the frequency shift <strong>of</strong> the first resonance �f are plotted<br />

over the bias voltage applied to the sample. The<br />

measurement was done at a maxima <strong>of</strong> the topography.<br />

[1] F. Bocquet et al., Phys. Rev. B 78, (2008), 035410.<br />

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