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AFM Basics Xinyong Chen.

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1 AFM Basics Xinyong Chen

2 Outline How AFM works Force measurements with AFM Scanning
Feedback control Contact mode and tapping mode Force measurements with AFM How AFM measures forces Calibrations Click for the Next

3 How AFM works Click for the Next

4 How AFM works Direct mechanical contact between the probe and the sampler surface Essential difference from traditional microscopy How AFM “feels” the surface topography? Optical level detection Click for the Next

5 Optical level detection
Voltage Difference Between Top & Bottom Photodiodes With this “split photodiode”, any slight vertical movement of the reflection spot position is detected by checking the difference between the “top” and the “bottom” photodiode dutputs (the “T-B signal”). (Click for the next) Top-Bottom Signal (V) or Deflection (nm) or Force (nN) Let’s split the photodiode into two – the “top” and the “bottom”. Assume that the optical reflection spot originally locates in the exactly middle of this split photodiode, resulting in the exactly same voltage output from the two photodiodes. So, the difference between the “top” (T) and the “bottom” (B) is zero. (Click for the next) During scanning, the sample surface may lift the cantilever up, resulting in corresponding move up of the optical reflection spot on the photodiode. However, this single photodiode couldn’t detect small position change of the spot. (Click for the next) Quad photodiode to detect Both vertical and horizontal Movements of the light spot. Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Cantilever + Sharp probe Photodiode Laser Scanner Photodiode Laser Scanner Click for the Next

6 How AFM works Direct mechanical contact between the probe and the sampler surface Essential difference from traditional microscopy How AFM “feels” the surface topography? Optical level detection Constant-height scan versus Constant-force scan Click for the Next

7 Constant-height scan Click for the Next
Click on graph to play animation (internet connection required)

8 Constant-height scan Advantages: Disadvantages:
Simple structure (no feedback control) Fast response Disadvantages: Limited vertical range (cantilever bending and detector dynamic range) Varied force Click for the Next

9 Constant-force scan Click for the Next
Click on graph to play animation (internet connection required)

10 Optical level detection in constant-force mode
In constant-force mode, whenever the sample surface topography would result in the cantilever deflection change, the other end of cantilever would be accordingly adjusted so that the cantilever deflection angle, and hence the contact force, would keep constant. Photodiode Laser Z scanner Cantilever + Sharp probe Photodiode Laser Z scanner Cantilever + Sharp probe Photodiode Laser Z scanner Cantilever + Sharp probe Click for the Next

11 Feedback control in constant-force mode
In constant-force mode, the cantilever’s vertical position is adjusted by an electronic feedback loop, with the T-B signal as the input and the vertical scanner voltage as the output. P.I.D. Control Horizontal Vertical Click for the Next

12 Constant-force scan vs. constant-height scan
Constant-height mode Constant-force mode Click for the Next Click on graph to play animation (internet connection required)

13 Constant-force scan vs. constant-height scan
Advantages: Large vertical range Constant force (can be optimized to the minimum) Disadvantages: Requires feedback control Slow response Constant-height Advantages: Simple structure (no feedback control) Fast response Disadvantages: Limited vertical range (cantilever bending and detector dynamic range) Varied force Click for the Next

14 How AFM works Direct mechanical contact between the probe and the sampler surface Essential difference from traditional microscopy How AFM “feels” the surface topography? Optical level detection Constant-height scan and constant-force scan Feedback control in constant-force scan Click for the Next

15 Sample swept by AFM probes
The constant AFM probe contact with the sample surface may cause damage of the sample, typically shown as “sweeping”. One of the techniques to avoid such a problem is the “tapping mode”. 1 mm Self-assembly of octadecyl phosphonic acid (ODPA) on single crystal alumina surface imaged in ethanol with tapping mode. The central 1 mm × 1 mm area was previously scanned in contact mode with heavy loading force. Click for the Next

16 Tapping mode AFM Click for the Next Click on graph to play animation

17 Feedback control in tapping mode
In tapping mode, the system uses the same feedback control as that used in constant-force contact mode. However, it usually uses the cantilever’s oscillation amplitude (the “AC” signal) instead of its DC component (the “Deflection”) as the input signal. P.I.D. Control Click for the Next

18 Tapping mode AFM PLA/PSA blend on Si imaged in air Height Phase 1 mm
In addition to the normal topographic image, tapping mode AFM can also provide simultaneously a “phase image” map, which results from variation in interactions between the AFM probe and the various sample surfaces. Click for the Next

19 How AFM works Direct mechanical contact between the probe and the sampler surface Essential difference from traditional microscopy How AFM “feels” the surface topography? Optical level detection Constant-height scan and constant-force scan Feedback control in constant-force scan Contact mode and tapping mode Click for the Next

20 Dimension AFM Click for the Next

21 MultiMode AFM Click for the Next

22 AFM Tips 80 – 320 mm 20 mm 35 mm 125 mm Click for the Next

23 AFM sample preparation
Click for the Next

24 AFM in liquid environment
One extraordinary feature of AFM is to work in liquid environment. A key point for liquid AFM is a transparent solid (usually glass) surface, which, together with the solid sample surface, retains the liquid environment whilst maintains stable optical paths for the laser beams. An optional O-ring can be used to form a sealed liquid cell. Otherwise, the system can also work in an “open cell” fashion. Click for the Next

25 Liquid AFM Images Click for the Next 70 nm
t=0 min 12 19 20 22 41 45 48 56 60 Effect of DNase I enzyme on G4-DNA (0.5:1) complex, the complex was immediately adsorbed onto mica and imaged until stable images were obtained, then the DNase I was introduced. Click for the Next Nucleic Acids Research, 2003, Vol. 31, No

26 Outline How AFM works Force measurements with AFM
Scanning and feedback control Contact mode and tapping mode Force measurements with AFM How AFM measures forces Calibrations Click for the Next

27 Force measurements with AFM
B C D (A+B)-(C+D) A+B+C+D Defl= P.I.D. Control When an AFM works in force measurement mode, the feedback loop is temporarily “cut off”. The cantilever deflection (the “T-B signal”) is then recorded while the AFM probe is vertically “ramped” towards/backwards the sample surface. (Click step-by-step to see how this is done.) Z Displacement Deflection Click for the Next

28 Experimental Force Curves
Contact slope to study hardness Adhesion to study intermolecular interactions Click for the Next

29 Calibration of force measurements
Slope = DD / DZ (V/nm) The Hooke’s law F = -kx Detector sensitivity S = Inverse of the contact slope measured on a hard surface (nm/V) Spring constant (N/m) Property of the cantilever and provided by the manufacturer Large variation due to difficulty in cantilever thickness control Should (and can) be experimentally measured for accuracy requirement Thermal fluctuation Resonance + geometry Mass adding + resonance Standard with known spring constant etc. T-B Signal Z Displacement (nm) x (V) Deflection (nm) DD Force (nN) DZ x Click for the Next

30 Humidity affects the adhesion
AFM probe Salbutamol Measurement of particle-particle interaction Lactose 1µm Force (nN) 200 400 600 800 1000 1200 <10% 22% 44% 65% ‘Nanoscale’ contact ‘Macroscale’ contact Click for the Next

31 Environmental AFM Both temperature and humidity can be controlled
in this environmental chamber. Click for the Next

32 Intermolecular interactions
MFP is specially designed for force measurement purpose MFP Schematic of the force–extension characteristics of DNA: at 65 pN the molecule is overstretched to about 1.7 times its contour length, at 150 pN the double strand is separated into two single strands, one of which remains attached between tip and surface. Click for the Next

33 Adhesion Force Imaging
Height Adhesion pH 7 Albumin Polystyrene PS Albumin Si 5 mm Click for the Next

34 Adhesion and Hardness Imaging
Height Adhesion Stiffness 1 mm PLMA/PmMl6 blend on Si imaged in water PLMA: poly (lauryl methacrylate) PmMl6: 2-methacryloyloxyethyl phosphorylcholine-co-lauryl methacrylate (1:6) Simultaneous Height, Adhesion and Stiffness maps are obtained with “Pulsed-Force” AFM technique. Click for the Next

35 Conclusions How AFM works Force measurements with AFM
Constant-height and constant-force scans (contact mode) Feedback control in constant-force mode Contact mode and tapping mode Force measurements with AFM Force curves: contact part to measure hardness and adhesion to measure intermolecular interactions Calibrations: Detector sensitivity (nm/V) = Inverse of contact slope on a hard surface => Convert the measured T-B signal (V) to cantilever deflection (nm) Spring constant (N/m) => Convert the cantilever deflection to force (N) [F=-kx] End


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