Transcript Document
X-ray diffraction
Antony D. Han
Chem 750/7530
Feb. 21, 2006
Outline
History
and background information of Xray diffraction.
Theory behind the equipment
Challenges of applying traditional XRD to
nano-technology
Summary
History of X-ray and XRD
Wilhelm Conrad Röntgen discovered
X-Rays in 1895.
1901 Nobel prize in Physics
Wilhelm Conrad Röntgen (1845-1923)
Bertha Röntgen’s Hand 8 Nov, 1895
A modern radiograph of a hand
History of X-ray and XRD
Radiographs like the ones in the
last slide are simply shadowgrams.
The X-rays either pass straight
through or are stopped by the
object. The diagram on the upper
left illustrates the principle and
shows a perfect shadow.
In reality, a large fraction of the Xrays are not simply absorbed or
transmitted by the object but are
scattered. The diagram on the
bottom left illustrates this effect and
illustrates the fuzzy edge of the
object that is produced in the image
by the scattered X-rays.
History of X-ray and XRD
The first kind of scatter process to be
recognised was discovered by Max von Laue
who was awarded the Nobel prize for physics
in 1914 "for his discovery of the diffraction of
X-rays by crystals". His collaborators Walter
Friedrich and Paul Knipping took the picture
on the bottom left in 1912. It shows how a
beam of X-rays is scattered into a
characteristic pattern by a crystal. In this
case it is copper sulphate.
The X-ray diffraction pattern of a pure
substance is like a fingerprint of the
substance. The powder diffraction method is
thus ideally suited for characterization and
identification of polycrystalline phases.
Max von Laue (1897-1960)
Bragg’s Law
Sir William Henry
Bragg (1862-1942)
William Lawrence
Bragg (1890-1971)
The father and son team of Sir
William Henry and William Lawrence
Bragg were awarded the Nobel prize
for physics "for their services in the
analysis of crystal structure by
means of Xrays“ in 1915.
Bragg's law was an extremely
important discovery and formed the
basis for the whole of what is now
known as crystallography. This
technique is one of the most widely
used structural analysis techniques
and plays a major role in fields as
diverse as structural biology and
materials science.
Equipment
Bruker D8 Analytical X-ray Systems
Goniometer
2-Theta:Theta Setup
Goniometer
Theta:Theta Setup
Fundamentals
How it works?
An electron in an alternating electromagnetic field will oscillate with the
same frequency as the field. When an X-ray beam hits an atom, the
electrons around the atom start to oscillate with the same frequency as
the incoming beam. In almost all directions we will have destructive
interference, that is, the combining waves are out of phase and there is
no resultant energy leaving the solid sample. However the atoms in a
crystal are arranged in a regular pattern, and in a very few directions we
will have constructive interference. The waves will be in phase and
there will be well defined X-ray beams leaving the sample at various
directions. Hence, a diffracted beam may be described as a beam
composed of a large number of scattered rays mutually reinforcing one
another.
Crystal systems, space groups, reciprocal lattice, Miller indices…
Planes going through areas with high electron density will reflect
strongly, planes with low electron density will give weak intensities.
Sample preparation
Single crystal X-ray diffraction
The single crystal sample is a perfect crystal (all unit cells
aligned in a perfect extended pattern) with a cross section of
about 0.3 mm.
The single crystal diffractometer and associated computer
package is used mainly to elucidate the molecular structure of
novel compounds.
Powder (polycrystalline) X-ray diffraction
It is important to have a sample with a smooth plane
surface. If possible, we normally grind the sample
down to particles of about 0.002 mm to 0.005 mm
cross section. The ideal sample is homogeneous and
the crystallites are randomly distributed. The sample
is pressed into a sample holder so that we have a
smooth flat surface.
Data collection and analysis
Collecting
data: computer and software
Analysis:
ICDD database – Identification
Structure refinement – GSAS
Quantitative phase analysis – GSAS
Novel structure – single crystal
Applications
Identification
Polymer
crystallinity
Residual stress
Texture analysis
Challenge of applying to
nanotechnology
Traditional X-ray powder-diffraction techniques rely on
the long-range order in crystals to produce sharp "Bragg
peaks" in a diffraction pattern. By examining these Bragg
peaks, which result from X-ray scattering, scientists can
determine the material's atomic structure.
But nanocrystals lack long-range order and often
incorporate a large number of defects. As a result, their
diffraction patterns are much more diffuse with few, if
any, Bragg peaks.
"This poses a real challenge to the traditional techniques
for structure determination," -- Valeri Petkov of Michigan
State.
Breakthroughs for diffraction
RTMS detection technology and the
implementation of mono-capillary have reduced
measurement times and minimum amounts of
material required considerably.
Many X-ray diffraction techniques are at disposal
of the nanoscientist now for the structural
characterization of the nanomaterials, such as
high-resolution diffraction, reflectometry, smallangle X-ray scattering and line profile analysis.
Summary
X-ray
diffraction provides a powerful tool to
study the structure and composition of the
materials which is a key requirement for
understanding materials properties
An X-ray diffraction system should not be
missing in a modern laboratory for
research on nano- and advanced
materials. – www.panalytical.com
Some useful links
GSAS:
http://www.ncnr.nist.gov/xtal/software/gsas.html
ICDD:
http://www.icdd.com/
CCP14
http://ccp14.sims.nrc.ca/
Diffraction tutorials
http://www.uniwuerzburg.de/mineralogie/crystal/teaching/basic.html
Paper addressed the problem
Phase Transitions, 2003, Vol 76, Nos. 1-2, pp. 171-185