X-ray diffraction: the basics

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Physics 590 1 X-ray diffraction: the basics Alan Goldman

Transcript of X-ray diffraction: the basics

Page 1: X-ray diffraction: the basics

Physics 590 1

X-ray diffraction: the basics

Alan Goldman

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What’s wrong with this picture?

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• atoms pack in periodic, 3D arrays • typical of:

Crystalline materials...

-metals -many ceramics -some polymers

What is the atomic scale structure?

• atoms have no “regular” packing • occurs for:

Noncrystalline materials...

-complex structures -rapid cooling

"Amorphous" = Noncrystalline

Distance between atoms ~ Å (10-10 m)

crystalline SiO2

noncrystalline SiO2 Adapted from Fig. 3.18(b), Callister 6e.

Adapted from Fig. 3.18(a), Callister 6e.

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Visible light

X-rays

Resolution ~ wavelength So, 10-10 m resolution Requires λ ~ 10-10 m

How do we use x-rays to study crystal structures?

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Different probes

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Different probes

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NEUTRONS X-RAYS ELECTRONS

Wavelength range 0.4 - 10 Å 0.1 - 5 Å 0 .04 - 0.2 Å

Energy range 0.001 - 0.5 eV 3000 - 100000 eV 6000 - 120000 eV

Cross-section 10-25 barns 10-25 Z2 barns ~10-22 barns

Penetration depth ~ cm ~ µm ~ nm

Typical flux 1011 s-1 m-2 1024 s-1 m-2 1026 s-1 m-2

Beam size mm-cm µm-mm nm-µm

Typical sample Any bulk sample Small crystals, powders, surfaces

Surfaces, thin films, grains, gases

Techniques Diffraction

Inelastic scattering Reflectivity

Diffraction Photon absorption

Photoemission Inelastic scattering

Microscopy Diffraction

Emission spectroscopy EELS

Phenomena

Magnetic/crystal structures

collective excitations (phonons, spin waves)

electronic excitations (crystal-field, spin-orbit)

Crystal structures, electronic transitions

(photoemission, absorption),

microstructure crystal structures

electronic transitions

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Why x-rays??

Easily accessible in the laboratory Penetration ~ microns to millimeters (tuned with energy)

Low-energies can be used to probe surface and near surface regions High energies can probe the bulk of a sample

High flux at National Facilities Allows you to throw a lot of photons away → high energy and

momentum resolution Is highly polarized and highly collimated Is continuously tunable across a wide range of energies (1 keV →

200 keV) Wavelength range ~ interatomic spacing (1-2 Å) → diffraction

interacts with electrons Magnetic interactions are higher order

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X-rays from a synchrotron source

Static charge ---- Electric field Charge moving at constant v ---- Magnetic field Accelerating charge --- Electromagnetic radiation

v

a

v << c v ≈ c

Synchrotron radiation is highly collimated highly linearly polarized highly brilliant continuous wavelength distribution (beyond Cu, Mo, etc..)

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Bending magnet radiation

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Places to go

Europe

AMES

SSRL

APS NSLS II

CHESS

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Advanced Photon Source

Synchrotron

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Insertion Devices

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Bragg’s Law –the view in real space

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But Physicists live in reciprocal space

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Diffraction peak intensities

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Whereas the dimensions and symmetry of the unit cell determine peak positions, peak intensities are governed by how the atoms are arranged within the unit cell.

Generally speaking:

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Single-crystal diffraction

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• Need to rotate through several angles • It’s easy to get “lost in reciprocal

space” • But you get a lot more detail!

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Scanning reciprocal space

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Flavors of samples

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Twinned crystals

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Is this just a nuisance?

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AE AE

Fe Fe As As

a b

Structural phase transition I4/mmm → Fmmm

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Strained samples

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Samples under pressure

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Mosaic crystals

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Ideal powder samples

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Powder diffraction

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ki kf

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Types of powder samples

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Fitting diffraction data

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Rietveld refinement Lattice constants space group Atom positions Site disorder/vacancies Thermal vibration amplitude Strain broadening R-factor

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X-ray resonant magnetic scattering*** Magnetic structures of neutron absorbing materials with very high

resolution

Pump-probe experiments Dynamics on picosecond to millisecond timescales

Inelastic x-ray scattering Approaching neutron energy resolution

X-ray absorption Spectroscopy*** Studies of local atomic environments and chemistry

Circular magnetic x-ray dichroism*** Element specific magnetization measurements

More than “just diffraction”

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Small–angle scattering Studying mesoscopic-scale structures

X-ray radiography and tomography 3D views of structural features with submicron resolution

Surface scattering Studies of both solid and liquid surfaces

Coherent x-ray diffraction Probing coherence effects on the atomic scale

More than “just diffraction”

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