introduction to powder diffraction/practical data collection · 2 [email protected]...
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Durham
ChemistryDepartment
DurhamUniversity
Introduction to Powder Diffraction/Practical Data
CollectionDr Ivana Evans
Durham, January 2007
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Outline
• Information in a powder pattern• What is diffraction• How to collect (laboratory) data• Lab vs synchrotron vs neutron• What is Rietveld refinement
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Session 2 – Introduction
2θ - degrees
Cou
nts
1. Peak positions determined by size, shape, symmetry of unit cell – internal
structure
2 9 .52 95
2. Peak Intensities determined by
where atoms sit in unit cell – internal
structure
3. Peak widths influenced by size/strain of crystallites -
microstructure.
2θ
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Historical background
1895: Röntgen discovers X-rays (Nobel Prize 1901)
1912: von Laue discovers X-ray diffraction on crystals (Nobel Prize1914)
1913: Bragg & Bragg discover structure analysis by XRD, NaCl (Nobel Prize 1915)
1916: Debye & Scherrer discover powder X-ray diffraction, LiF
1963: Zachariasen solves the structure of β-Pu from PXRD by direct methods
1969: Rietveld method
1990: direct space approaches to structure solution
2000: work on 100+ atom structures, proteins
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[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Diffraction: physical phenomenon
Crystalline state of matter• long-range 3D orderDiffraction• scattering on periodic arraysCrystallography• 2dhklsinθ = λ• Fhkl = Σfje2πi(hxj+kyj+lzj)
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Samples
2-theta
I
(a) (b)
(d)(c)
Single crystal
Four differently oriented single crystals
Polycrystalline material
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[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Experiment
2θ
2θ
‘…data compressed into one dimension…’
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Powder diffraction can give you
Powder DiffractionPowder Diffraction
Thermal expansion
Particle sizePhase
transitions
Ionic migration
PolymorphismIn-situ
chemistry
Particle strain
Structure determination
Kinetics studies
Crystallization/amorphization
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Laboratory Configurations
(a)(b)
1
2
4
5 16
2
33
2θθ
Reflection geometry Transmission geometry
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Laboratory Bragg Brentano
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Laboratory Bragg Brentano
Tube
Divergence Slits/Sollers
Sample
AntiscatterSlits/Sollers
ReceivingSlit
Mono-chromator
Detector
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PSD for Speed
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Capillary Transmission Mode
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Sample Preparation
• Dependent on experiment• Bulk holders• Single crystal Si wafers for low background• See examples on guided tour
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[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Data Collection
• Machine dependent• Make sure statistics are good enough for information you
need• Consider spending longer counting at higher 2θ to
compensate for intensity fall off in diffraction• Make sure you have sufficient points to define a peak (e.g.
10 across fwhm) – can rebin later but can’t create extra points
• Consider optical set up and whether it’s suited for your sample (see later tutorials)
• First guess on a “normal” lab instrument– 5-90º 0.02º step, 1 second per step ~ 1 hr
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Common Crimes – Sample Prep
• Surface roughness• Intensities affected as f(2θ)• “Negative temperature factors”
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[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Common Crimes – Sample Prep
• Sample height
2θ offset = zero - 2*∆height*cos(θ)/radius;
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Common Crimes – Sample Prep
• Infinite thickness• e.g. organic sample sprinkled on substrate
may not be infinitely thick• Intensities affected as f(2θ)
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[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Common Problems – Sample Prep
• Preferred orientation• e.g. platelets with c-axis perpendicular to
sheets will give strong 00l reflections• Might be able to correct
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Common Problems – Sample Prep
• Texture• Much harder to correct• Certain unrelated hkl reflections wrong
intensity
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[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Avoiding Preferred Orientation
• Capillary measurements• Flat plate reflection & transmission• Side/back mounting• Spray drying• Sieving• Neutron diffraction
http://www.ccp14.ac.uk/solution/powdermounts.htm
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Common Crimes – Data Collection
• Beam overspill• Intensities affected as f(2θ)• High background at low 2θ due to sample holder
High 2θ Low 2θ
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[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Common Crimes – Data Analysis
• LP Factors – don’t ignore the geometry of the instrument you’re using
• Different configurations require different corrections
• e.g. Bragg-Brentano, incident monochromator
θθθθ
cossin2cos2cos1
2
22monoLP +
=
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Common Crimes – Data Analysis
• Think about errors!• Poisson statistics sig(I)=I0.5 normally assumed• No longer true if you scale data • No longer true for psd’s where some parts of
pattern measured for longer• Use 2θ, I, sig(I) format – error propagation!
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[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Synchrotron vs Lab
• Pros– Far higher intensities– Choice of wavelength– Much sharper peak widths– Grenoble/Didcot/Japan/etc
• Cons– Sample damage– Must apply for beam time– Limited access– Grenoble/Didcot/Japan/etc
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Neutrons vs X-rays
• Pros– Distinguish e.g. Mn/Fe– Information on O in metal oxides– Penetrating so can use complex sample environment– Grenoble/Didcot/Japan/etc
• Cons– Flux generally much weaker than X-rays– Large samples– Must apply for beam time– Limited access– Grenoble/Didcot/Japan/etc
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[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Refinement: pre Rietveld
Integrated intensity refinement• State of the art until late 60’s early
70’s
• Poor observation-to-parameter ratio
• Problems due to overlap
• Limited applicability
• Suitable for high symmetry systems
• Used extensively for high T nonstoichiometric phases
12 observations
4 variables• Scale factor• Uiso(Fe)• Uiso(O)• Occ(O)
Cheetham et al., 1971.
[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Refinement: the Rietveld method
Rietveld, 1969: diffraction pattern analysis by a curve fitting procedure
First proposed for constant wavelength neutron data
The difference between the observed and calculated profiles is minimized
• typical Rietveld plot:
Parameters refined:
• structural parameters (atomic positions,displacement parameters, occupancies,unit cell parameters)
• instrumental parameters (zero point, background parameters)
• peak shape function parameters
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[email protected] www.durham.ac.uk/ivana.radosavljevic PCG workshop January 2007
Conclusions
• Overview/intro to diffraction/Rietveld• Many specific details will be covered in later
lectures/tutorials• Tour of instruments if you want