Electric Force Microscopy (EFM)
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Model: EFM-2017
In EFM, a conductive cantilever tip is used an sample is prepared with surface potentials on it is needed. The tip and sample are separated a distance z usually by air or vacuum. A bias voltage between tip and sample is applied by an external voltage supply that forming a capacitor, C, between tip and sample. The capacitance of the system depends on the geometry of the tip and sample. The total energy stored in that capacitor is U = 1/2C*ΔV^2. The w ork done by the voltage supply to maintain a constant voltage, ΔV, between the capacitor plates (tip and sample) is -2C*U. The z component of the force (the force along the axis connecting the tip and sample) is thus:

When the tip scans the surface of a sample at close distances (< 5 nm), not only long range electrostatic forces are sensed, but also van der Waals force, atomic interaction forces. In order to reduce topography artifact in the EFM image, a second path of scan at lifted distance from the surface topography is implemented. The commercial implementation of this method is so-called “Lifting” method.

SPECIFICATIONS
| Scan Size | Scanner Dependent |
| Scan Rate | 0.1 -2 Hhz |
| Lift Magnitude* | 0 – 10 V |
| Lift Ramp Rate* | 19.5 V/Msec |
| Drop Ramp Rate* | 19.5 V/Msec |
| Interscan Delay | 0 – 10000 msec |
| Field Amplitude | 0-100% |
| Bias Voltage | 0-10V |
| Vibrating Mode Fr. | 20-600 Khz |
| Probe | Conductive |
*Multily X Gain in nm/V to convert from volts to nanometers
INCLUDE WITH EFM OPTION
- Conductive Porbes
- Power Supply
- Software
- Sample Holder
- Manual
Power Supply

A power supply is used to directly supply a biast to the probe or the sample.
Interface Unit

In the EFM image acquisition tab, the topography image is displayed at the right and the EFM image is displayed at the right.
