AFM University Introduction to Atomic Force Microscopy by Paul West

« Cover
« Foreward
« Chapter 1
 « Chapter 2
 
2.1. Basic Concepts
2.2. The AFM Stage
2.2.1 XYZ Scanners
2.2.2 Force Sensors
2.2.3 Integrating LL-Force Sensors and Scanners
2.2.4 Z Motors-Probe Approach
2.2.5 X-Y Stage
2.2.6 Optic Microscope
2.2.7 Mechanical Loop
2.3 Electronics
2.4 AFM Acquisition Software
2.5 LL-AFM Cantilevers and Probes
2.6.1 Vibrations
2.6.2. Environmental Scanning
2.6.3 Heating/Cooling Stages
2.6.4 Higher Speed AFM Scanning
 « Chapter 3
 « Chapter 4
 « Chapter 5
 « Chapter 6
 « Chapter 7
« Appendix A
« Appendix B
« Appendix C
« Appendix D
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Chapter 2


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2.2.4 Z Motors-Probe Approach
One of the major challenges in an AFM is making a motion control system that allows moving the probe to the surface before scanning. This must be done such that the probe does not crash into the surface and break. An analogous engineering challenge would be to fly from the earth to the moon in 60 seconds and stop 38 meters from the surface with out overshooting or crashing.
In the AFM stage there are two separate motion generation mechanisms in the Z axis. The first is a stepper-motor-driven mechanism with a dynamic range of a centimeter and a resolution of a few microns. The stepper motor is driving either a linear bearing or an 80 TPI screw. The second motion generation mechanism in the Z axis is the piezoelectric ceramic in the AFM scanner. The z ceramic typically has a dynamic range of about 10 microns or less and a resolution of less than 0.5 nm.
FIGURE 2-20 Motion of probe in the “woodpecker” method for probe approach in an atomic force microscope. The z PZT and Z motor are activated sequentially until the surface is detected.
Typically, probe approach is achieved with a “woodpecker” method, Figure 2-20. In this method, the stepper motor is stepped a small increment, say 1 micron. Then the z piezoelectric ceramic is extended 5 microns to see if the surface is detected. The z piezo is then retracted, the stepper motor engaged.......on and on. A key component here is that when the probe encounters the surface, the feedback is turned on immediately.
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