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Stanford Synchrotron Radiation Laboratory
X-ray ScatteringMike Toney
Stanford Synchrotron Radiation Laboratory
(00Qz) (20Qz)(-10Qz)
• J Als-Nielsen & D McMorrow, “Elements of Modern X-ray Physics”, Wiley (2001).
• M. Tolan, “X-ray Scattering from Soft-Matter: Materials Science and Basic Research”, Springer, 1998.
• RL Snyder, K. Fiala &HJ Bunge, Eds., “Defect and Microstructure Analysis by Diffraction”, Oxford (1999).
• G Renaud, “Oxide Surfaces and Metal/Oxide Interfaces Studied by Grazing Incidence Diffraction”, Surf Sci Repts 32, 1 (1998)
Bibliography
1. Peak Widths & Defects• Nanoparticles
2. Monoatomic Layers – Pentacene again3. Surface Diffraction
• Oxide Surfaces• Interfacial Water
4. Small Angle X-ray Scattering (SAXS)
Outline
Diffraction vs Scattering
0 20 40 60 80
1000
2000
3000
4000
5000
6000
7000
21 24 27
2000
4000
6000
Inte
nsity
2θInte
nsity
2θ
diffraction: Bragg peaks
scattering: the rest
Peak Widths
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
37.4 37.6 37.8 38 38.2 38.4 38.6 38.8 39 39.2
2 Theta
Inte
nsity
(111)
• Widths depend on particle size (D):∆2θ = 0.9 λ / D cos θ∆Q = π/D
∆2θ = 0.15deg => D = 50 nm
Nanoparticles
Kevin Stevens (MPT Solutions, NZ)Bridget Ingham (Imperial College, UK)Simon Brown (U Canterbury, NZ)
Cu particles nanoscaleparticles, formed by inert gas aggregation, are deposited from a molecular
Peak Widths
Cu particles: a = 3.6159 +/- 0.0005 Å(c.f. bulk 3.6149 Å)D = 12 nm compared to 30-60 nm from SEM
Cu2O (cuprite): ca 5% by volume
Monolayer Scattering
(00Qz) (20Qz)(-10Qz)
monoatomic layer of atoms
monoatomic layer of molecules
1 1.2 1.4 1.6 1.8 2 2.2 2.4
qxy (Å-1)
Inte
nsity
(a.u
.)
(11)
(02)(12)
(20) (21)
0.05 0.1 0.15 0.2 0.25 0.3 0.35
qz (Å-1)
Inte
nsity
(a.u
.)
peak (11)peak (12)peak (02)
Pentacene Monolayer
2θα
β
Transport in ab plane of crystal structureTransport in first few layers
Fritz et al., unpublished
• Monolayer: herringbone motif with molecules untilted
• lattice parameters (monolayer)a = 5.911 (3) Åb = 7.566 (3) Åγ = 90.0 (1)o
• Thin film:a = 5.933 (3) Åb = 7.540 (3) Åγ = 90 deg
5µm
a
bγ
Fritz et al., unpublished
Pentacene Monolayer
Pentacene revisited
0.007 Å-1
width
Fritz et al., unpublished
5 µm 1.5 nm - one layer
30 nm – ca 15 layers
5 µm
5 µm=> Grain size of > 30 nm
Surface ScatteringRECIPROCAL
SPACEREAL
SPACE
Infinite lattice results in pointsin reciprocal space.
A single plane of atoms resultsin lines of intensity.
Surface is combination.
Surface Scattering
CTR: crystal truncation rod
IK Robinson PRB 33, 3830 (1986).
A. Munkholm, S. Brennan & E.C. Carr, J. Appl. Phys. 82, 2944 (1997).
sum over all Bragg peaksnearest Bragg peak only
202 CTR
Hydrated Oxide Surface StructureSurface XRD to probe
Eng et el., Science 288, 1029 (2000)
α-Al2O3 (0001)
(00Qz) (20Qz)(-10Qz)
Hydrated Oxide Surface Structure
Some hydrated surface structures
Eng et el., Science 288, 1029 (2000)Trainor et el., Surf Sci 496, 238 (2002)Trainor et el., Surf Sci (2004)
Interfacial Water Structure
positively charged surface
negatively charged surface
oxygen
hydrogen• microscopic picture of the arrangement of water at oxide-aqueous interfaces
Surface X-ray Diffraction or Crystal Truncation Rods (CTRs)
Interfacial Water Structure
Toney et al., Nature 368, 444 (1994)
-ve of pzc
Ag(111)
+ve of pzc
(00Qz) (20Qz)(-10Qz)
Interfacial Water Structure
-(ve) charged surface
+(ve) charged surface
Small Angle Scattering
|Q| = (4π/λ)sin (θ/2)Kin
KoutQ = Kout - Kin
θKin
incident scattered
Measure I(Q) with Q ∼ 0.0001 – 1 Å-1
Scattering from density inhomogeneitiesof size 0.5 – 1000 nm
Small X-ray Angle Scattering Intensity
ρ1(2) = electron densityin phase 1(2)
pores = particles
23riQ rd e)r(
V1I(Q) •∫= ρ ρ(r) = electron density
S(Q)F(Q))(VNI(Q) 22
12 ρρ −=
single particleSAXS
inter particlescattering
∫ •
1V
3riQ rd e
Small Angle ScatteringIsolated pores or particles with diameter D
• Experimental Q range gives range of accessible diameters• Need 1/D Q 10/D<~ <~
π/D
Q-4
Inter-pore Interference: S(QR)
S(QR) = interference function using local mono-disperse approximation (positions correlated with size)JS Pederson, J Appl. Cryst. 27, 595 (1994)
SAXS from nearby pores interfere
Sample
2D Area Detector
• Sample to detector distance defines Q range (for a given λ)
• Q = (4π/λ) sin(θ/2)• Two or three detector distances
(0.1m to 3m) & incident beam sizes
• Gives large Q range• Performed in transmission• Window-less environment
θ
Incident X-Ray BeamMonochromate to E=7.66 keV,Slits: 100 x 100 or 200 x 200 µm
80 µm Si substrate transmission~25%
SAXS Setup
Spin coat MSSQ/Porogensolution
Heat to 450°C, at5°C/min under argon
Cool to room temperature
1.
2.
3.Thermally
Labile Polymer
Methyl Silsesquioxane(MSSQ), CH3SiO1.5
SiO
O
CH3
O
O Si
CH3
SiCH3
Si
CH3
O
O
O
O
∆ Argon
Porogens: copolymer poly(methyl methacrylate-co-dimethylaminoethyl methacrylate) or P(MMA-co-DMAEMA) & poly(ε-caprolactone) or PCL (6-armed star)
Matrix
Components Processing
Spin Coat
MSSQ crosslinks at 200°CPoragen fully degrades at 400°C
Nanoporous Films
Porogen
Small Angle X-ray Scattering
• MSSQ matrix• P(MMA-co-DMAEMA) porogen• Loading = weight percent in initial
material• Porosity is about 90% of loading• Fits with local monodisperse
model and log-normal distribution
Huang et al, Appl. Phys. Lett. 81, 2232 (2002)
Pore Size DistributionApproximations:
treat pores as spheres (ignore shape)local mono-disperse approximation for inter-pore scattering
5.45.340%
4.54.530%
3.12.715%
2.62.110%
D/2 (nm)
<R> (nm)
loading
σ ≈ 0.37
Nanoporous Films
Reconstruction of Pore Morphology
Allows determination of transition from closed pores to open pores to bicontinuous microstructure
Hedstrom et al, Langmuir20, 1535 (2004)
Nanoporous Films
=> transition to bicontinuous occurs between 15 & 25 %
closed and interconnected:number ∼ length3
bicontinuous:number ∼ length2
Grazing Incidence SAXS
2θ
incident scattered
• Use grazing incidence to limit penetration depth• Measure I(Q) with Q ∼ 0.01 – 1 Å-1
• Scattering from density inhomogeneities of size 50 – 100 Å
Applications:• Nanoparticles imbedded in
thin films• Nanoparticles on surfaces
k
k’
= (4π/λ) sin θQ = k’ – k
Summary
1. Peak Widths & Defects• Nanoparticles
2. Monoatomic Layers – Pentacene again3. Surface Diffraction
• Oxide Surfaces• Interfacial Water
4. SAXS applications to porous and particulate materials