B. S. Swartzentruber 1
Characterization of Nanomaterials
Brian S. Swartzentruber, CINT Science Dept.
…from atoms to nanostructures, ensemble systems, and devices
Characterizing nanostructure properties is critical for detailed understanding, predictability, and control.
• Structure properties• Electronic properties
Bulk and interface transportElectronic structureSurface effects
• Mechanical propertiesElastic and plastic deformationFracture and failure mechanisms
• Kinetic propertiesProcesses underlying formation, organization, stability, and decayDiffusivity and diffusion mechanisms
100
101
102
103
104
J (A
/cm
2 )
-0.4 -0.2 0.0 0.2 0.4
Bias (V)
37 nm 54 nm 73 nm 104 nm
250 nm
B. S. Swartzentruber 2
STM can probe atom-scale motion directly
Brian Swartzentruber, 844-6393
r
r2
r1
adatom
L
A meandering localized defect enables the adatom to diffuse via hopover.
Temperature dependence yields the activation barrier.
1.24 eV
Distinctive features of the statistics of motion – a nonbinomial jump distribution, a nonexponential wait-time distribution, and direction and time correlations – imply 1-d hopover diffusion.
w/ Ezra Bussmann
B. S. Swartzentruber 3
AFM provides rapid characterization of surface nanostructures
Julia Hsu, 284-1173
topographycurrent
A
4 m
Carbon fiber in insulating polymer matrix
160 nm
0
250 nmTop of zinc oxide nanorods
B. S. Swartzentruber 4
Conducting AFM enables correlation between topography and conductance
Julia Hsu, 284-1173
Investigate percolation transport of carbon nanofiber - polyimide (insulating polymer) composite microscopically using CAFM.
electrode
Current passes through carbon nanofiber network only (not all nanofibers are part of network).
currenttopography
4 m 4 m4 m
w/ Aaron Trionfi
B. S. Swartzentruber 5
Julia Hsu, 284-1173
Piezoelectric force microscopy (PFM) relates mechanical and electrical state of materials
Polymer
Nanorod Au coatpAamplifier
Biasvoltage
Tipi
250 nm
Topo
PFM
160 nm
7 pm/V0
0
Embedded zinc oxide nanorods
Resistivity (Ωcm)
d 33 R
espo
nse
(pm
/V)
The piezoelectric response correlates directly with the resistivity of the nanorods.
PFM Current
500 nm
w/ David Scrymgeour
B. S. Swartzentruber 6
Interfacial Force Microscopy (IFM) has a non-compliant force sensor that eliminates “snap-to-contact”
Jack Houston, 844-8939
A complete force profile – approach and retract – for a diamond tip on a NaCl crystal. The tip ‘attaches’ to the salt at DC and, upon retraction, pulls out a nanowire that breaks at DR.
The force sensor uses two capacitors in a ‘teeter-totter’ configuration to balance the force.
xyz PiezoController
Sample
ProbeCommon Plate
and Torsion Bars
Cantilever AFM behavior
w/ Nathan Moore
B. S. Swartzentruber 7
The Tecnai F30 TEM at CINT contains specialized piezo-controlled probes
Jianyu Huang, 284-5963
TEM-STM
TEM-AFM
TEM-Indenter
Pulling a nanowire from the NaCl substrate in real time shows the fast diffusion kinetics, defect density, and recrystallization.
B. S. Swartzentruber 8
The ‘air-free’ TEM allows transfer through a glove-box without contamination
Todd Monson, 845-2129
Magnetic nano-particles can be synthesized and imaged in an air-free environment before transfer for magnetic characterization.
TB
B. S. Swartzentruber 9
Nanomanipulator in an SEM allows electrical characterization and direct manipulation of nanostructures
Brian Swartzentruber, 844-6393
Nanomanipulator current-voltage measurements yield metal-semiconductor interface character.
100
101
102
103
104
J (A
/cm
2 )
-0.4 -0.2 0.0 0.2 0.4
Bias (V)
37 nm 54 nm 73 nm 104 nm
Rods are rectifying with diameter-dependent behavior.
Probe contacts Au catalyst particle for IV measurement through the Ge rod.
5
4
3
2
1
n
200150100500
Diameter (nm)
Idea
lity
fact
or
Theoretical ‘carrier-recombination’ mechanism has ideality factor of two.
Rods of diameter > 75 nm appear bulk-like. Depletion width increases in smaller rods.
Forward-bias exponential slope yields ‘ideality factor’.
Ge rods are grown from Au catalyst in a variety of sizes.
w/ Alec Talin
B. S. Swartzentruber 10
Nanomanipulator in an SEM allows electrical characterization and direct manipulation of nanostructures
Brian Swartzentruber, 844-6393
Joystick positioning and programming command allow precise placement and motion control.
500 nm
250 nm
Pulling probe from salt crystal plastically deforms outer layer.
Electron beam ‘shadow’ helps position probe.
Advantage: complete flexibility in hardware, software, and data acquisition
100 nm GaAs rod
Tip-nanostructure adhesion allows pick-and-place.
B. S. Swartzentruber 11
Designing micro-scale platforms for testing mechanical, thermal, and electrochemical properties
John Sullivan, 845-9496
gap for sample
Thermal driven force actuator
Calibrated load measurement
CINT Cantilever Array Discovery Platform™Mechanical Properties
20 m
• Thermal & electrical properties of nanoscale materialsThermal Properties
Electrochemical Properties• Real-time imaging
of electrochemical processes with nanoscale resolution
• Electrochemical cell that operates inside a TEM
seals
electrode 1 window electrode 2
electrolyte channel
Cyn
thia
Vol
kert
(Uni
vers
ity o
f G
oetti
ngen
, Ger
man
y)20
08 C
INT
Use
r Pro
ject
B. S. Swartzentruber 12
Pulsed field gradient nuclear magnetic resonance (PFG-NMR) measures the diffusion of nanoparticles in solution
Todd Alam, 844-1225
Self diffusion and molecular motion of liquids in nano-materials can be measured. Details about the impact of morphology on transport properties within nano-composites and the assembly of nanoparticles and dendrimers are determined.
Decay of NMR signal as a function of field gradient yields particle diffusivity.
PFG NMR - Au Nanoparticles
Gradient (G/cm)
0 5 10 15 20 25 30
Nor
mai
lzed
Sig
nal I
ntes
ity
0.2
0.4
0.6
0.8
1.0
rs
6skTrD
Organically Capped NanoparticlesPFG NMR - Au Nanoparticles
Gradient (G/cm)
0 5 10 15 20 25 30
Nor
mai
lzed
Sig
nal I
ntes
ity
0.2
0.4
0.6
0.8
1.0
rs
6skTrD
Organically Capped Nanoparticles
Present Sandia investigations include:• Diffusion measurements of H2O within fuel cell membranes. How do
changes in membrane nano-morphology (domain size, pore size and surface modification) control the transport rates?
• Measurement of transport in porous materials, and impact of nanostructure on transport of different molecular species
• Measurement of the interaction and aggregation between surface modified nanoparticles and the impact of diffusion of these assemblies.
B. S. Swartzentruber 13
Low-energy electron microscope (LEEM) can image real-time surface nano-structure formation and self-assembly processes
Gary Kellogg, 844-2079
4
Pb/Cu(111)
Pla
ss e
t al.
Patterns are thermodynamic, arising from stress difference between the two phases.
But kinetics have to be fast enough to allow the patterns to form!
Low-energy electron microscope (LEEM) images of Pb/Cu(111)
4
Increasing Pb coverage
• Spatial resolution: 7-8 nm• Time resolution: video rates• Sample temperature: 150 K -1800 K• Background pressure: UHV• Contrast mechanisms: work function
differences (surface chemistry, doping differences), electron interference (surface steps), electron diffraction (surface reconstructions), etc.
Overlayer white - Alloy black
B. S. Swartzentruber 14
LEEM images show p-n contrast on device test structures
Gary Kellogg, 844-2079
10 μm FOV, 0.90 μm linen-type p-type
Blanket n-type implant (<1017)
p-type(~1019)
1000 μm
n-type lines
Schematic of test structure LEEM image of p-n interface
n-type
p-type
=1.2 V
Start Voltage (V)
Inte
nsity
(arb
. uni
ts)
Ramping incident electron energy yields information on surface potential, doping, and oxide properties.
w/ Meredith Anderson
B. S. Swartzentruber 15
Microsystems reliability and failure analysis is pushing to the nanoscale
David Stein, 845-8476
• Charge-Induced Voltage Alteration (CIVA)• Low Energy CIVA (LECIVA)• Light-Induced Voltage Alteration (LIVA)• Seebeck Effect Imaging (SEI)• Thermally-Induced Voltage Alteration (TIVA)
Measure voltage fluctuations in a constant-current power supply as an electron or photon beam is scanned across an IC.
Soft Defect Localization (SDL)
FIB for Imaging and Circuit Editing
TIVA Defect Isolation
• Expertise in Si CMOS, III-V, MEMS, and Optoelectronics
• Support throughout the product life cycle • Extensive reliability & failure analysis capabilities, equipment, tools & techniques
TIVA and STEM for Optoelectronic Failure Analysis
SEM + Nanoprober to arrive fall ‘08
B. S. Swartzentruber 16
Characterizing nanostructure properties is critical for detailed understanding, predictability, and control
• STM can probe atom-scale motion directly• AFM provides rapid characterization of surface nanostructures• Conducting AFM enables correlation between topography and conductance• Piezoelectric force microscopy (PFM) relates mechanical and electrical state of
materials• Interfacial Force Microscopy (IFM) has a non-compliant force sensor that eliminates
“snap-to-contact”• The Tecnai F30 TEM at CINT contains specialized piezo-controlled probes• The ‘air-free’ TEM allows transfer through a glove-box without contamination• Nanomanipulator in an SEM allows electrical characterization and direct manipulation of
nanostructures • Designing micro-scale platforms for testing mechanical, thermal, and electrochemical
properties• Pulsed field gradient nuclear magnetic resonance (PFG-NMR) measures the diffusion of
nanoparticles in solution• Low-energy electron microscope (LEEM) can image real-time surface nano-structure
formation and self-assembly processes • LEEM images show p-n contrast on device test structures• Microsystems reliability and failure analysis is pushing to the nanoscale
David Stein, 845-8476
Gary Kellogg, 844-2079
Gary Kellogg, 844-2079
Todd Alam, 844-1225
John Sullivan, 845-9496
Brian Swartzentruber, 844-6393
Brian Swartzentruber, 844-6393
Todd Monson, 845-2129
Jianyu Huang, 284-5963
Jack Houston, 844-8939
Julia Hsu, 284-1173
Julia Hsu, 284-1173
Julia Hsu, 284-1173
Contact information is on the poster.