ATOMICFORCEMICROSCOPY
1
Ahsan Bukhari.
799-2020
ATOMIC FORCE MICROSCOPY
• AFM WORKS BY SCANNING A PROBE OVER THE SAMPLE
SURFACE, BUILDING UP A MAP OF THE HEIGHT OR
TOPOGRAPHY OF THE SURFACE AS IT GOES ALONG.
BACKGROUND OF AFM
3
⚫In 1929 Shmalz described Stylus Profiler.
⚫In 1950 Becker suggested oscillating the probe that
approach contact with surface.
⚫In 1971 Young described non contact type Stylus Profiler.
⚫In 1981 Binning and Rohrer described STM.
⚫AFM Invented in 1986 by Binning.
DIFFERENT FROM OTHER
MICROSCOPY
4
⚫No need of focusing, illumination, Depth of field.
⚫It also have height information that make it simple to
quickly measure the height, volume, width of any feature
in the sample.
⚫It physically feels the sample’s surface with a sharp probe,
building up a map of the height of samples surface.
⚫It provides single atomic level structure so provide high
resolution.
THE FIRST AFM INSTRUMENT BUILT
BY BINNING, QUATE AND GERBER
5
The STM with a lever
made by carefully gluing a
tiny diamond onto the end
of a spring made of a thin
strip of gold. This was the
cantilever of the first AFM.
AFM INSTRUMENT
6
The main components of an AFM are
1.Microscope stage – Moving AFM tip, Sample holder,
Force Sensor
2.Control electronics - Optical Microscope, Vibration
controller
3.Computer - The control electronics usually takes the form
of a large box interfaced to both the microscope stage and
the computer.
BASIC CONCEPT OF AFM
INSTRUMENTATION
7
The piezoelectric transducer moves the tip over the
sample surface, the force transducer senses the force
between the tip and the surface, and the feedback
control feeds the signal from the force transducer back in
to the piezoelectric, to maintain a fixed force between the
tip and the sample.
PIEZOELECTRIC
TRANSDUCERS
8
amorphous lead barium titanate,
Convert electrical potential into mechanical
PdBaTiO3
motion.
or lead
zirconate titanate, Pb[ZrxTi1–x]O3,0<x<1
FORCE
TRANSDUCERS
9
It may beconstructed that measure forces as lowas 10
piconewtons.
FORCE
SENSOR
10
Optical lever sensor the
End of the cantilever
bends the position of
the laser spot on the
detector changes. As the
cantilever detector
distance is large a small
movement of the
cantilever causes a large
change in the laser spot
position at the detector.
FEEDBACK CONTROL
FEEDBACK CONTROL IS USED TO MAINTAIN A SET FORCE BETWEEN THE
PROBE AND THE SAMPLE.
12
CHALLENGES OF AFM
REGARDING DESIGN
13
⚫Requirement of sharp probe for high resolution.
⚫The force between probe and sample should be 1nN or
less than that.
⚫The feedback controller should have a rapid control so
adjust topographic film can be formed.
⚫A high speed computer that can generate the images in
real time.
⚫Vibration free stage.
SCANNING MODES
14
There are different imaging modes of AFM
 Contact Mode
 Non Contact Mode
 Tapping Mode
MODES OF OPERATION
IN AFM
15
Mode of Operation
⚫Contact mode strong(repulsive) -
Force of Interaction
constant force or
constant Height
⚫Non-contact mode weak (attractive) -
⚫Tapping mode strong (repulsive) -
vibrating probe
vibrating probe
CONTACT
MODE
16
⚫High Resolution Images.
⚫Tip of the probe always touching the sample.
⚫Fastest of all the topographic modes.
⚫Because of repulsive forces tip and sample may damage.
⚫Sensitive to the nature of sample.
⚫Not good for soft samples.
NON CONTACT MODE
⚫ SIGNAL-TO-NOISE BENEFITS ASSOCIATED WITH MODULATED SIGNALS.
⚫ OSCILLATING MODES CAN MEASURE IMAGES WITH A SMALL PROBE–
SAMPLE FORCE.
TAPPING MODE
⚫ NO CAPILLARYEFFECT.
⚫ AMPLITUDE SIGNALS ARE USED IN FEEDBACK.
⚫ USED FOR IMAGING IN AIR.
LIMITATIONS
⚫ AFM CAN ONLY IMAGE A MAXIMUM HEIGHT ON THE ORDER OF 10-20
MICROMETERS AND A MAXIMUM SCANNING AREA OF ABOUT
150×150 MICROMETERS.
⚫ THE SCANNING SPEED OF AN AFM IS ALSO A LIMITATION.
⚫ HIGHLY DEPENDENT ON AFM PROBES.
APPLICATIONS
21
⚫It can image far more biological processes, such as
imaging of proteins.
⚫Any sample like ceramic material, human cells or
individual molecules of DNA, Dispersion of metallic
Nanoparticles can be imaged.
REFERENCES
22
⚫Atomic force Microscopy by Peter Eatson and Paul West.
⚫http://hansmalab.physics.ucsb.edu/afmapp.html
⚫QuazarTechnologies Pvt., LTd. Guide section.
THANK YOU
23

Atomic Foce Microscopy by Syed Ahsan Bukhari.pptx

  • 1.
  • 2.
    ATOMIC FORCE MICROSCOPY •AFM WORKS BY SCANNING A PROBE OVER THE SAMPLE SURFACE, BUILDING UP A MAP OF THE HEIGHT OR TOPOGRAPHY OF THE SURFACE AS IT GOES ALONG.
  • 3.
    BACKGROUND OF AFM 3 ⚫In1929 Shmalz described Stylus Profiler. ⚫In 1950 Becker suggested oscillating the probe that approach contact with surface. ⚫In 1971 Young described non contact type Stylus Profiler. ⚫In 1981 Binning and Rohrer described STM. ⚫AFM Invented in 1986 by Binning.
  • 4.
    DIFFERENT FROM OTHER MICROSCOPY 4 ⚫Noneed of focusing, illumination, Depth of field. ⚫It also have height information that make it simple to quickly measure the height, volume, width of any feature in the sample. ⚫It physically feels the sample’s surface with a sharp probe, building up a map of the height of samples surface. ⚫It provides single atomic level structure so provide high resolution.
  • 5.
    THE FIRST AFMINSTRUMENT BUILT BY BINNING, QUATE AND GERBER 5 The STM with a lever made by carefully gluing a tiny diamond onto the end of a spring made of a thin strip of gold. This was the cantilever of the first AFM.
  • 6.
    AFM INSTRUMENT 6 The maincomponents of an AFM are 1.Microscope stage – Moving AFM tip, Sample holder, Force Sensor 2.Control electronics - Optical Microscope, Vibration controller 3.Computer - The control electronics usually takes the form of a large box interfaced to both the microscope stage and the computer.
  • 7.
    BASIC CONCEPT OFAFM INSTRUMENTATION 7 The piezoelectric transducer moves the tip over the sample surface, the force transducer senses the force between the tip and the surface, and the feedback control feeds the signal from the force transducer back in to the piezoelectric, to maintain a fixed force between the tip and the sample.
  • 8.
    PIEZOELECTRIC TRANSDUCERS 8 amorphous lead bariumtitanate, Convert electrical potential into mechanical PdBaTiO3 motion. or lead zirconate titanate, Pb[ZrxTi1–x]O3,0<x<1
  • 9.
    FORCE TRANSDUCERS 9 It may beconstructedthat measure forces as lowas 10 piconewtons.
  • 10.
    FORCE SENSOR 10 Optical lever sensorthe End of the cantilever bends the position of the laser spot on the detector changes. As the cantilever detector distance is large a small movement of the cantilever causes a large change in the laser spot position at the detector.
  • 11.
    FEEDBACK CONTROL FEEDBACK CONTROLIS USED TO MAINTAIN A SET FORCE BETWEEN THE PROBE AND THE SAMPLE.
  • 12.
  • 13.
    CHALLENGES OF AFM REGARDINGDESIGN 13 ⚫Requirement of sharp probe for high resolution. ⚫The force between probe and sample should be 1nN or less than that. ⚫The feedback controller should have a rapid control so adjust topographic film can be formed. ⚫A high speed computer that can generate the images in real time. ⚫Vibration free stage.
  • 14.
    SCANNING MODES 14 There aredifferent imaging modes of AFM  Contact Mode  Non Contact Mode  Tapping Mode
  • 15.
    MODES OF OPERATION INAFM 15 Mode of Operation ⚫Contact mode strong(repulsive) - Force of Interaction constant force or constant Height ⚫Non-contact mode weak (attractive) - ⚫Tapping mode strong (repulsive) - vibrating probe vibrating probe
  • 16.
    CONTACT MODE 16 ⚫High Resolution Images. ⚫Tipof the probe always touching the sample. ⚫Fastest of all the topographic modes. ⚫Because of repulsive forces tip and sample may damage. ⚫Sensitive to the nature of sample. ⚫Not good for soft samples.
  • 17.
    NON CONTACT MODE ⚫SIGNAL-TO-NOISE BENEFITS ASSOCIATED WITH MODULATED SIGNALS. ⚫ OSCILLATING MODES CAN MEASURE IMAGES WITH A SMALL PROBE– SAMPLE FORCE.
  • 18.
    TAPPING MODE ⚫ NOCAPILLARYEFFECT. ⚫ AMPLITUDE SIGNALS ARE USED IN FEEDBACK. ⚫ USED FOR IMAGING IN AIR.
  • 20.
    LIMITATIONS ⚫ AFM CANONLY IMAGE A MAXIMUM HEIGHT ON THE ORDER OF 10-20 MICROMETERS AND A MAXIMUM SCANNING AREA OF ABOUT 150×150 MICROMETERS. ⚫ THE SCANNING SPEED OF AN AFM IS ALSO A LIMITATION. ⚫ HIGHLY DEPENDENT ON AFM PROBES.
  • 21.
    APPLICATIONS 21 ⚫It can imagefar more biological processes, such as imaging of proteins. ⚫Any sample like ceramic material, human cells or individual molecules of DNA, Dispersion of metallic Nanoparticles can be imaged.
  • 22.
    REFERENCES 22 ⚫Atomic force Microscopyby Peter Eatson and Paul West. ⚫http://hansmalab.physics.ucsb.edu/afmapp.html ⚫QuazarTechnologies Pvt., LTd. Guide section.
  • 23.