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AFM at Video Rate and Beyond Frontiers in Scanning Probe Microscopy, Purdue University, October 2006 Mervyn Miles H.H. Wills Physics Laboratory IRC in Nanotechnology University of Bristol Tyndall Avenue Bristol U.K. IRC in Nanotechnology

AFM at video rate and beyond

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Page 1: AFM  at video rate and beyond

AFM at Video Rate and Beyond

Frontiers in Scanning Probe Microscopy,Purdue University, October 2006

Mervyn Miles

H.H. Wills Physics LaboratoryIRC in Nanotechnology

University of BristolTyndall Avenue

BristolU.K.

IRC inNanotechnology

Page 2: AFM  at video rate and beyond

High-resolution 3-D imaging;

Imaging in liquid, air, & vacuum;

No staining or coating required;

No radiation damage;

Mapping of physical properties;

Modification of surfaces;

Non-scanning applications: force spectroscopy, sensors, ...

Atomic Force Microscopy: Strengths

Page 3: AFM  at video rate and beyond

Speed Weakness of SPM

Imaging rate too low:

to follow many processes;

to examine large areas of a specimen;

to create or manipulate structures over usefully large areas.

Page 4: AFM  at video rate and beyond

Scanning system ~ inertia and resonance problems

Feedback loop response time

Response of interaction sensor

Force-sensing cantilever has inertia and resonance

L i m i t a t i o n s o f C o n v e n t i o n a l S P M

General to all SPMs

S p e c i f i c t o A F M

Page 5: AFM  at video rate and beyond

Parallel imaging with multiple cantilevers

Strobe imaging of repetitive processes

Decrease Q in AC modes

Shift the time domain using higher frequencies

Another method ....

How to go faster:

Page 6: AFM  at video rate and beyond

S o l u t i o n 1

Decrease the mass of the scanning system

Increase the stiffness of the scanning system

Decrease the mass of the cantilever

Increase the stiffness of the cantilever

Decrease the Q factor of the cantilever

Page 7: AFM  at video rate and beyond

Instead of avoiding resonance,

use a resonating beam

for scanning in the fast direction

A Different Solution

Page 8: AFM  at video rate and beyond

S o l u t i o n 2

Scan by oscillating at resonance with a high amplitude - resonant scanning microscopy (RSM);

High Q-factor results in high scan stability;

Data are collected throughout each sweep;

Page 9: AFM  at video rate and beyond

Before high-speed AFM,

we first built a high-speed SNOM

Page 10: AFM  at video rate and beyond

Specimen

scan

OpticalDetector Optical fibreQuartz Tuning Fork

(Drive & feedback)

Capture & ProcessingElectronics

Feedback Control

Scanning Near-field Optical Microscopy (SNOM)

Exponential decay of evanescent field away

from the interface

ADL Humphris, JK Hobbs, MJ Miles, Applied Physics Letters, 83(1), 6-8 (2003)

Page 11: AFM  at video rate and beyond

Melt-tapered optical fibre SNOM probe

Page 12: AFM  at video rate and beyond

Specimen

scan

OpticalDetector Optical fibreQuartz Tuning Fork

(Drive & feedback)

Capture & ProcessingElectronics

Feedback Control

Scanning Near-field Optical Microscopy (SNOM)

Exponential decay of evanescent field away

from the interface

ADL Humphris, JK Hobbs, MJ Miles, Applied Physics Letters, 83(1), 6-8 (2003)

Page 13: AFM  at video rate and beyond

LaserDetector

Probe

Transverse dynamic force microscope (TDFM)

IRC inNanotechnology

Page 14: AFM  at video rate and beyond

Low-amplitude (~1 nm) Oscillations

Page 15: AFM  at video rate and beyond

Transverse Dynamic Force Microscope, TDFM

M Antognozzi

Page 16: AFM  at video rate and beyond

-1 -0.5 0 0.5 1 1.5 2 2.5 3 3.5 4tip-sample distance (nm)

0

0.2

0.4

0.6

0.8

a bPROBE PROBE

SAMPLE SAMPLE

Surface detection via confined water layer

M Antognozzi, ADL Humphris, MJ Miles, APPLIED PHYSICS LETTERS, 78(3), 300-302 (2001)

Page 17: AFM  at video rate and beyond

Low-amplitude (~1 nm) Oscillations

Page 18: AFM  at video rate and beyond

High-amplitude (~ 5 µm) for fast axis scanning

Tip scanning in fixed plane set by average optical intensity

For high-speed SNOM

ADL Humphris, JK Hobbs, MJ Miles, Applied Physics Letters, 83(1), 6-8 (2003)

Page 19: AFM  at video rate and beyond

Several crystals may nucleate together and grow to forma spherical structure known as a spherulite.

Spherulite

Within the spherulite, the polymer crystals grow radially from the centre in a ribbon morphology

These ribbon crystals often twist as they grow with the same pitch and remain in phase.

In a thin film, the spherulite is a disk-like structure in which the coherent twisting of the ribbon crystals results in concentric rings

with the ribbons alternately flat on and edge.

Page 20: AFM  at video rate and beyond

5 µm5 µm

Crystallization of poly(hydroxybutyrate-co-valerate) (PHB/V)

Quality factor has been reduced from 270 to 90. Tip velocity was 403µm/s, line rate 8Hz

AFM

Topography Phase

Page 21: AFM  at video rate and beyond

High Amplitude Oscillations

Page 22: AFM  at video rate and beyond

Birefringent PSTM

Shear-force controlledvia tuning fork

2 µm Height

2 µm Optical

P

A

Slow scanning - 20 minutes/imageassisted with active Q

Detector

Polariser

Analyser

ADL Humphris/JK Hobbssee, e.g., RL Williamson, MJ Miles, JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B, 14(2), 809-811 (1996

Page 23: AFM  at video rate and beyond

High Amplitude Oscillations

Page 24: AFM  at video rate and beyond

Conventional SNOM1 frame in 1000 sec

RSM SNOM120 frames/sec

PHB spherulite between crossed polars

Comparison:Conventional SNOM & RSM SNOM

200 nm

> 100,000 Faster than existing SNOM

ADL Humphris, JK Hobbs, MJ Miles, Applied Physics Letters, 83(1), 6-8 (2003)

Page 25: AFM  at video rate and beyond

High-speed SNOM of collagen

Intensity related to height - 67 nm repeat of collagen visible

A Major (Uni Wien, ), L Bozec, MA Horton, Miles

Page 26: AFM  at video rate and beyond

Specimen

scan

OpticalDetector

Optical fibre

Quartz Tuning Fork(Drive & feedback)

Capture & ProcessingElectronics

Feedback Control

Scanning Near-field Optical Microscopy (SNOM)

transmission

Analyzer

Polarizer

A. Ulcinas, M Antognozzi

Page 27: AFM  at video rate and beyond

piezo drivers operating in tandem

` flexures

sample stage

Flexure Stage for high-speed SPM

This flexure stage provides the high-speed scan of up to 40kHz with about 3 µm amplitude

Picco, Engledew

Page 28: AFM  at video rate and beyond

High-speed SNOM of polymer spherulite of PHB

Flexure stage scanner - 3 µm x 3 µm imageTransmission SNOM with crossed polars

A. Ulcinas, M Antognozzi, Picco, Engledew

Page 29: AFM  at video rate and beyond

High-speed AFM

Page 30: AFM  at video rate and beyond

Resonant scanning AFM

conventional scan tube

cantilever

piezo stack (y)

QCR (x)

top

side Resonant sample scan stage (x)

Piezo stack for ‘slow’ scan (y)

No electronic feedback

Mechanical feedback

super lubricity

water in confined geometry

ADL Humphris, MJ Miles, JK Hobbs, Applied Physics Letters, 86(3), Art.No. 034106 (2005)

Page 31: AFM  at video rate and beyond

High-speed AFM of Chitosan Film

30 frames/s(Infinitesima vAFM)

Ulcinas, Payne, Heppenstall-Butler1µm x 1µm

Conventional AFM

> 3000 Faster than conventional AFM

- tuning-fork resonance scanning

Page 32: AFM  at video rate and beyond

piezo drivers operating in tandem

` flexures

sample stage

Flexure Stage for high-speed SPM

This flexure stage provides the high-speed scan of up to 40kHz with about 3 µm amplitude

Picco, Engledew

Page 33: AFM  at video rate and beyond

PEO Spherulite video AFM

30 frames/second1.5 µm x 1.5 µm

Engledew, Picco, Miles

- flexure stage (non-resonance) scanning

Page 34: AFM  at video rate and beyond

Engledew, Picco, Miles

PEO Spherulite video AFM

30 frames/second

- flexure stage (non-resonance) scanning

Page 35: AFM  at video rate and beyond

30 frames/second1.5 µm x 1.5 µm Engledew, Picco, Miles

PEO Spherulite video AFM

Page 36: AFM  at video rate and beyond

0 mins0 frames

10 mins18,000 frames

3 mins~ 6000 frames

7 mins13,000 frames

PEO video AFM 30 f/s - image reproducibility

Page 37: AFM  at video rate and beyond

High-speed AFM of ‘large’ objects

Page 38: AFM  at video rate and beyond

Air c AFM

Picco, Miles, Komatsubara, Hoshi, Ushiki

Set of human chromosomes

Page 39: AFM  at video rate and beyond

Picco, Miles, Komatsubara, Hoshi, Ushiki

Human Chromosome No. 2

Page 40: AFM  at video rate and beyond

Picco, Miles, Komatsubara, Hoshi, Ushiki

Page 41: AFM  at video rate and beyond

Picco, Miles, Komatsubara, Hoshi, Ushiki

Air

High-speed AFM of parts of human chromosomes

Picco, Miles, Komatsubara, Hoshi, Ushiki

Page 42: AFM  at video rate and beyond

Picco, Miles, Komatsubara, Hoshi, Ushiki

Montage of high-speed AFM images of part of human chromosome No. 2

Page 43: AFM  at video rate and beyond
Page 44: AFM  at video rate and beyond

Picco, Miles, Komatsubara, Hoshi, Ushiki

Air

Page 45: AFM  at video rate and beyond

Picco, Miles, Komatsubara, Hoshi, Ushiki

2M NaCl

Page 46: AFM  at video rate and beyond

Picco, Miles, Komatsubara, Hoshi, Ushiki

2M NaCl

Human chromosomes in liquid

Height range: ~0.5 µm

Page 47: AFM  at video rate and beyond

Conventional AFM Image of Collagen Specimen

Page 48: AFM  at video rate and beyond

Collagen Fibres

Banding periodicity: 67 nm

30 fps Picco, Bozec, Horton Engledew

Page 49: AFM  at video rate and beyond

Conventional AFM

High-speed AFM

All the high-speed images were taken in 0.7 s

Linear Collage of High-speed AFM Images of Collagen Fibre

Page 50: AFM  at video rate and beyond

Single frame from collagen movie

Image acquired in 17 msPicco, Bozec, Horton Engledew

Page 51: AFM  at video rate and beyond

High-speed AFM Collagen Collage

12 images involved - acquired in 200 msPicco, Bozec, Horton Engledew, Miles

Page 52: AFM  at video rate and beyond

Large area collagen collage

103 images acquired in 1.7 s

Page 53: AFM  at video rate and beyond

Non-imaging:

High-speed writing

Electrochemical oxidation of passived silicon

Page 54: AFM  at video rate and beyond

Local AFM electrochemical oxidation

Can be used to pattern surface -conventional AFM too slow to pattern large areas

Page 55: AFM  at video rate and beyond

250 nm

10 ms; -12 V Si tip; conventional AFM

non-contact

Ti Oxidation James Vicary

Page 56: AFM  at video rate and beyond

Topographic AFM images of oxide nanostructures created with a -12 V tip bias for pulse times. Height range: 2 nm.

100 µs

50 µs

10 µs

5 µs

1 µs

500 ns

Oxidation of Silicon with high-speed AFM

Picco, Vicary

Page 57: AFM  at video rate and beyond

High-speed AFM

Simultaneous writing (oxidation) and imaging

3 voltage pulses synchronized to fast line scan

30 fps

Read-Write

Picco, Vicary

Page 58: AFM  at video rate and beyond

Conventional AFM of oxidized lines on Si

Page 59: AFM  at video rate and beyond

How fast can this system image?

9 fps 15 fps 30 fps

High-speed AFM of Collagen

30 fps50751002505007501000>1000

AFM images in less than 1 ms

Bimorph Tuning fork Flexure

Page 60: AFM  at video rate and beyond

`

piezo drivers operating in tandem

tuning fork scanning

Scanner Arrangement for kilohertz AFM

Page 61: AFM  at video rate and beyond

500 nm x 500 nm

Collagen

Playback slowed down by > 40 times!

Frame Rate:

1300 fps

Line Rate:

64,000 lps

Each frame acquired in: 750 µs

PlaybackRate:25 fps

Collagen banding 67 nm

1 Million Images generated in ~15 minutes!Picco, Ulcinas, Antognozzi, Engledew, Horton, Bozec, Miles

Page 62: AFM  at video rate and beyond

CollagenFrame Rate:

1200 fps

Line Rate:

64,000 lps

Specimen being oscillate by 50 nm

500 nm x 500 nm

PlaybackRate:25 fps

Collagen banding = 67 nm

Picco, Ulcinas, Antognozzi, Engledew, Horton, Bozec, Miles

Page 63: AFM  at video rate and beyond

Composite image from 1000 fps AFM of Collagen

200 nm

Page 64: AFM  at video rate and beyond

So far, the movies were rather pixellated ....

... this can be fixed by increasing the line rate further ....

Page 65: AFM  at video rate and beyond

Picco, Ulcinas, Antognozzi, Engledew, Horton, Bozec, Miles

Frame Rate:1000 fps

Line Rate:

200,000 lps

PlaybackRate:25 fps

200 x 100 pixels; ~ 25 ns/pixel (on average)

Page 66: AFM  at video rate and beyond

Nanoscience and QI Centre, Bristol

Thanks to...

i

Peter Dunton Massimo AntognozziMonica BerryDebra BrayshawDavid EngledewSimon HawardJon Hayes(Jamie Hobbs)(Andy Humphris*)Terry McMaster

(Andras Major)Sheila MorrisLoren PiccoAndy Round Mark SzczelkunArturas UlcinasJames VicaryCraig WilliamsAlex Wotherspoon

Infinitesima

Niigata University:Tatsuo UshikiOsamu HoshiNae Komatsubara

UCL, London :Michael HortonLaurent Bozec

*www.infinitesima.com Thank you for your attention