Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford...

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Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7 th Annual SSRL Scattering School An Overview

Transcript of Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford...

Page 1: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Small Angle X-ray Scattering

Christopher J. Tassone

Stanford Synchrotron Radiation Lightsource

Materials Science Department

7th Annual SSRL Scattering School

An Overview

Page 2: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Outline

Overview of SAXS:

• Beamline Nuts & Bolts

• Calculating q-range

• SAXS Fundamentals and Scattering Patterns

• Real World Science Examples

• Moving into the future

- In-operando

- Probing materials off equilibrium

- In-situ growth

Page 3: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Beamline Nuts and Bolts

Page 4: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Calculating q-range

λ = 2dsin(θ)

Q = 2π/d

Easiest way to do this is to find your q/pixel

D S θpix

Xs-d

Xpix

To do this you need: •Detector Pixel Size

•Sample to detector distance

•Energy of incident x-ray photons

•Beamstop Size

•Detector Size

1) Solve for θpix

θpix = tan-1(xpix/xs-d)

2) Convert θpix to qpix

qpix = 4πsin(θpix)/λ

3) Find first real pixel p1= (rbstop/xpix)

4) qmin= qpix * p1

5) qmax= qpix * pdet/2

Page 5: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

SAXS Fundamentals

Fundamentally looking at form factor scattering only:

I(q) = F(q)2Z(q)2

I(Q) = ∫Γn(r)e-iqrdr

Scattering from 1-100 nm density

inhomogeneities

k

2q

incident

scattered

k’

Q

Page 6: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

SAXS Fundamentals

Fundamentally looking at form factor scattering only:

I(q) = F(q)2Z(q)2

I(Q) = ∫Γn(r)e-iqrdr

Scattering from 1-100 nm density

inhomogeneities

k

2q

incident

scattered

k’

Q

Page 7: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Understanding SAXS Profiles

• Guinier regime:

gives Rg, which is a measure

for the size of the particles

• Porod exponent:

provides

information about

shape of the

particles

polydisperse in

shape and/or size

Page 8: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Understanding SAXS Profiles

monodisperse in

shape and size

Form factor:

• depends on geometrical

shape of particles

• gives size and electron

density distribution of

particles

Page 9: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Understanding SAXS Profiles

Structure factor:

• Sequence of peaks Symmetry of structure

• Position of peaks Size of structure

• Width of peaks Size of domains/grains

• Intensity of peaks Degree of crystallinity

• Azimuthal distribution of peaks Orientation of domains

periodic

structures

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Science at Beamline 1-5

Block-co-polymers

Mesoporous Materials

Nanomaterial Synthesis

Nanoparticle Characterization

Batteries/Energy Storage

Catalysts

Energy Generation Materials

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Science Highlight-BCP Ordering

Rao, et. Al. Adv. Mater. 2010, 22, 5063. www.elitenetzwerk.bayern.de

Can we use BCP for:

• Improved transport in oFETs?

•Membranes for ionic transport?

Organic Electronics •Flexible

•Low cost

•Facile processing

•Light weight

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Science Highlight-BCP Organization

Understanding BCP Phase Diagram through SAXS

Ho, Victor; Boudouris, B.W.; McCulloch, B.L.; Shuttle, C.G.; Burkhardt, M; Chabinyc, M.L.; Segalman, R.A. “Poly (3-alkylthiophene) Diblock

Copolymers wuth Ordered Microstructures and Continuous Semiconducting Pathways” J. Amer. Chem Soc. 133, 2011, 9270.

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Science Highlight-BCP Templated Nanoparticle Films

Electrochemical

Charge Storage

TiO2 H2O

OH-

H2O

O2

O2-

CO2

+ Organic

Precursors Catalysts

Photovoltaics

Adv. Mater. 2011, 23, 3144

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Science Highligh-BCP Templated Nanoparticle Films

Me

erw

in’s

Salt

BC

P

inco

rpo

ration

Film

Co

nd

en

sa

tion

Th

erm

al

Annealin

g

Rauda, I.E.; Saldariaga-Lopez, L.C.; Helms, B.A.; Schelhas, L.T.; Membreno, D.;

Milliron, D.J.; Tolbert, S.H. “Nanoporous Semiconductors Synthesized Through

Polymer Templating of Ligand-Stripped CdSe Nanocrystals.” Adv. Mater. 25, 2013.

1315.

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PEO Domain

Aromatic Domain

Inter-domain

spacing

Inter-molecular

spacing

Domain

size

How Does Membrane Morphology Relate to

Ionic Conductivity?

•Use SAXS to characterize nano and

mesoscale morphology as a function of

PEG loading

•Random co-polymer PEO-PI

•Conductivity peaks when PEG loading

is high enough to observe PEO-PEO

domain correlations (20 nm)

Science Highlight-Random co-polymer Membranes

Page 16: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Controlling BHJ Morphology

Thermal

Annealing Increases

crystallinity

Increases phase

segregation

Solvent Additives Increases crystallinity

Increases or decreases phase segregation

More isotropic crystal distribution

No Post Processing

Solvent

Annealing Increases

crystallinity

Increases phase

segregation

Page 17: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Processing Additives Tune Morphology Uniquely

Processing additives… •enhance crystallinity

•increase isotropic distribution

of crystallites

•can increase or decrease

degree of phase segregation

Pure CB DIO

Liang, Y. et. Al. doi:10.1002/adma.200903528

OT Pure oDCB

J. Rogers et al., doi: 10.1021/ja2104747

Y.Yao et. al. doi:10.1002/adfm.200701459

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How Does Solution Behavior Effect Solid Film

Formation?

Page 19: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

How Does Solution Behavior Effect Solid Film

Formation?

?

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Probing Solid State Film and Casting Solution

Solution SAXS

Solid State SAXS

Page 21: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Interpreting SAXS Data

Two Regimes •Guinier domain size

•Porod •Diffuseness of interface

between domains

•Shape of aggregate

Page 22: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Probing Solid State Film

Solution SAXS

Solid State SAXS

Page 23: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Processing Additives Decrease Phase Segregation

-2.7

-3.5

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Visualizing Morphologies

Representative 3D morphologies

B. Ingham et al., doi:

10.1107/S00218898110048557

no additive

w/ ClN

w/ DIO

w/ ODT

Page 25: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Probing Casting Solution

Solution SAXS

Solid State SAXS

Page 26: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

C16-PDPP2FT Solution Phase Conformation

10-4 10-3 10-2 10-110-3

10-2

10-1

1

101

102

103

104

105

106

Inte

nsi

ty[a

.u.]

q [Å-1]

41 kDa

36 kDa

29 kDa

23 kDa

q-3

q-1

‡‡

a)

Low Mn High Mn

b)

10-4 10-3 10-2 10-110-3

10-2

10-1

1

101

102

103

104

105

106

Inte

nsi

ty[a

.u.]

q [Å-1]

41 kDa

36 kDa

29 kDa

23 kDa

q-3

q-1

‡‡

a)

Low Mn High Mn

b)

Page 27: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

Chloronapthalene has little effect on PCBM Aggregation

Neat CB

Increasing Concentration

Neat CB 5% CN

Page 28: Small Angle X-ray Scattering · Small Angle X-ray Scattering Christopher J. Tassone Stanford Synchrotron Radiation Lightsource Materials Science Department 7th Annual SSRL Scattering

10-4 10-3 10-2 10-110-3

10-2

10-1

1

101

102

103

104

105

106

Inte

nsi

ty[a

.u.]

q [Å-1]

41 kDa

36 kDa

29 kDa

23 kDa

q-3

q-1

‡‡

a)

Low Mn High Mn

b)

Putting Together Polymer and Fullerene Behavior

5% CN

Neat CB

K. Schmidt. Adv. Mater. doi:10.1002/adma.201303622

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Mechanism Summary

1. Additive promotes ordering within solution phase aggregates

2. PCBM stays well dispersed in solution with or without additive

3. Films cast with additive show small more intermixed domains

Weakly ordered polymer aggregates act as dispersed seed

sites for crystallization during film formation

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Enabling Science Through Beamline Upgrades

• Characterization of disordered soft

materials

• Fuel cell membranes

• Organic Photovoltaics

• Bioelectronics

• Anatomical materials

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Increasing In-situ Capabilities

• Increased in-situ capabilities

• Solution phase reactor

• Electrochemical fluid cell

- Battery materials

- Catalyst materials

- Electrochemical Capacitors

• Stress-strain curves

Dogbone

Force Transducer

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In-situ Printing at BL 1-5

Print Film

Collect SAXS/WAXS

Extract Metrics

Change Printing

Conditions