- A -
3d-AFM
ac-EFM
ac
Electrostatic Force Microscope In
ac-EFM the cantilever is made to oscillate by
an ac potential that is applied to the sample at the
resonant frequency of the cantilever. This produces
an ac force on the cantilever proportional to the
local ac potential Vs(w)
beneath the tip. The resulting oscillation amplitude
is recorded using an external lock-in amplifier; the
signal is proportional to Vs(w) .
Phys. Rev. Lett. 84, 6082 (2000).
Acoustic microscope
Atomic force microscope enabling one to image the
topography of a sample, and to monitor simultaneously
ultrasonic surface vibrations in the MHz range. For
detection of the distribution of the ultrasonic vibration
amplitude, a part of the position-sensing light beam
reflected from the cantilever is directed to an external
knife-edge detector.
Appl. Phys. Lett. 64, 1493 (1994)
AFM
Atomic
Force Microscope AFM
is type of Scanning
Probe Microscope (or Scanning
Proximity Microscope) with a microscopic force
sensor as a probe. By scanning the AFM force
sensor (flexible cantilever with the tip on the end)
over a sample surface (or scanning a sample under
the cantilever) and recording the deflection of the
cantilever, one can measure the local height, chemical
and mechanical properties of a sample.
Phys.Rev.Lett.56, 930 (1986).
AGC
A-HFM
Amplitude
HFM (Heterodyne Force Microscopy), see
HFM
AMFM
Attractive-mode force microscope.Mode
of operation of a quartz tuning-fork-based dynamic
mode atomic force microscope for the imaging of biological
samples under ambient conditions. AMFMuses a stiff
cantilever that maintains stable oscillations at low
amplitudes even in the presence of capillary and other
long range forces that can overwhelm more flexible
cantilevers.
Rev. Sci. Instr. 72, 4261 (2001).
ARTM
AFM
ASD
Amplitude
Slope Detectionn Measuring
a force derivative by deriving a shift in the cantilever
resonance frequency from a change in the cantilever
vibration amplitude driven at constant frequency.
J. Appl. Phys. 61, (1987) 4723.
aNFOM
apertureless
NFOM This
technique is based on measuring the modulation of
the scattered electric field from the end of a sharp
silicon tip as it is stabilized and scanned in close
proximity to a sample surface. The demonstrated resolution
lies in the 3 nm range—comparable to what can be achieved
with typical attractive mode atomic force microscopes.
Appl. Phys. Lett. 65, 1623 (1994).
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