Department of Physics, University of Siegen · Department of Physics, University of Siegen ......
Transcript of Department of Physics, University of Siegen · Department of Physics, University of Siegen ......
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Department of Physics, University of Siegen
Modern experimental methods for crystal structure determination and refinement
Lecture course on crystallography, 2015*** ***THIS LECTURE CONTAINS OPTIONAL MATERIAL
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1895: Discovery of X-rays by W.C Roentgen
Wilhelm Conrad Röntgen
The discovery of a new radiation type, which can easily pass through the substances.
1895
1901
Nobel prize in physics
"in recognition of the extraordinary services he has rendered by the discovery of the remarkable rays subsequently named after him"
Röntgen rays = X-rays
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Generation of X-rays
+ -
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The amazing properties of X-rays to be invisible to a human eye but penetrate easily through
matter remained unexplained for some time.
One of the hypotheses was suggesting that X-rays are the
electromagnetic waves with the wavelength much shorter than the wavelength of visible light.
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1912: Discovery of X-ray diffraction by crystals
Max von Laue 1912
1914
Nobel Prize in Physics
"for his discovery of the diffraction of X-rays by crystals"
1912 is the birth of Solid State Physics
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Spectrum of electromagnetic waves
Do X-rays have the same (wave) nature as visible light?
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1912: The experiment of Max von Laue
X-ray beam Crystal
Photographic film X-ray tube
An X-ray beam was directed onto a copper sulphate crystal. The experiment was performed by Friedrich
and Knipping
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Original experimental setup of Laue, Friedrich und Knipping
X-ray tube
Photographic film
Collimator Crystal
Exhibited in Deutsches Museum, München
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Laue pattern: diffraction of X-rays by a crystal
The first Laue pattern: diffraction of X-rays on a CuSO4 crystals obtained by Max von Laue,
Friedrich and Knipping
A modern Laue pattern: diffraction of X-rays on
quartz (SiO2) crystal
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The BASIC physical principles of X-ray diffraction
X-rays are electromagnetic waves with the wavelength of the order l=1 Å (10-10 m)
X-rays are scattered by electrons (Thomson scattering)
The waves scattered at different crystal sites interfere with each other. The sum of two waves depends on the phase difference
between them
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Interference / diffraction of waves Interference of light is a physical phenomena occurring when two
waves of the same wavelength sum up with each other. One defines CONSTRUCTIVE and DESTRUCTIVE interference
Important parameter: phase shift between wave 1 and wave 2
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Newton rings
R
Path difference, d
1
2
Waves 1 and 2 overlap with each other at the phase shift, d
d = 2p d / l
1
2
R
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Further examples
1
2
2 d sin q = n l
q q
l
Substrate
Thin film
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Physical principle of scattering techniques*
r 1E
2 1 1 0exp( 2 ( ) )i p= E E k k r
Suppose that a monochromatic X-ray beam with wavelength l hits a crystal. The primary beam is described by the wave vector k0 the scattered beam is described by the wave vector k1 . The length of both wave vectors is 1/l
The sum of the electric field vectors from the waves scattered at electrons 1 and 2 is
1 0 1 1 0 1 1 0 1 0( , ) 1 exp(2 ( ) exp(2 ( ) exp(2 ( )i i ip p p= = A k k E k k r E k k 0 k k r
k0
0E
k0
k1
k1 2
Phase difference between
waves 1 and 2
the amplitude of scattering depends on the DIFFERENCE between the wave vectors
1
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Scattering vector and scattering angle*
k0
k1 H
2θ
The amplitude of X-ray scattering is usually described as a function of a scattering vector H (instead of k1 and k0). Replacing two separate scatters (see previous page) by distributed density:
( ) exp 2A i dV p= H r Hr
With (r) being an ELECTRON DENSITY so that (r)dV is the amount of electrons in the small volume dV. The intensity of the X-ray scattering is the square of the absolute value of electric field so that
2( ) ~| ( ) |I AH H
H = k1 - k0 Scattering vector
Scattering angle
𝐻 = 2 ∙𝑠𝑖𝑛𝜃
𝜆
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Scattering by a crystal (periodic system)* Consider the scattering amplitude, A(H), for the periodic crystal. In this case electron density can be described by LATTICE and UNIT CELL
( )
( ) ( )exp(2 ) exp(2 )uvw
uvwunitCELL
A i dV i p p= H r Hr HA
Contribution of the single UNIT CELL (F) CRYSTAL LATTICE (L)
( ) r
( ) ( )uvw = r r A
a
b
Auvw
Lattice translation
The sum (integration) over the whole crystal can be reduced to the integration over the single unit cell only:
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Contribution of the crystal lattice*
( ) exp(2 )uvw
uvw
L ip= H HA The sum is carried out over all lattice points
It is convenient to decompose the scattering vector by the reciprocal lattice basis, a* b* and c* so that H= h a* + k b* + l c*. In this case the dot product
between vectors H and A is reduced to
( ) exp(2 ) exp(2 ) exp(2 )u v v
L ihu ikv ilwp p p= H
It can be easily shown that in the case of an X-ray beam that illuminates Na Nb and Nc unit cells in the directions a b and c then
2 2 22
2 2 2
sin ( ) sin ( ) sin ( )( )
sin ( ) sin ( ) sin ( )
a b cN h N k N lL hkl
h k l
p p p
p p p=
LAUE INTERFERENCE FUNCTION
HAuvw = hu + kv + lw
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Laue interference function*
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Laue interference function*
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Laue interference function*
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Conclusion: LAUE EQUATION The intensity of scattering by a crystal is non-zero for the scattering vectors H whose reciprocal lattice coordinates are integers. That means, the scattering from a crystal (with a given lattice) is described by the corresponding RECIPROCAL LATTICE
LAUE EQUATION for the diffraction by a crystal
k1 - k0 = h a* + k b* + l c*
h, k and l are indices of reflection
SCATTERING DIFFRACTION
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Contribution of the UNIT CELL* Electron density in the unit cell is the sum of the electron densities of the constituting atoms. Suppose that atoms occupy the sites in the unit cell at the positions R1, R2, ... Rn. Each atom has its own electron density around the nucleus position. We suppose that electron density of a single / isolated atom m is m(r)
1
( ) ( )n
m mm
=
= r r R
a
b
R1
R2 R3
( ) ( )
( ) ( )exp(2 ) ( )exp(2 )unitCELL unitCELL
F i dV i dVmm
p p= H r Hr r R Hr
The scattering amplitude by the single unit cell is then given by
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( ) ( )exp( )f i dVm m p= H r Hr
Atomic scattering factor depends only on the type of atom m and can be calculated for each atom in the periodic table
ATOMIC SCATTERING FACTOR
Atomic scattering factor is the amplitude of the X-ray scattering by a single (isolated) atom
Electron density of single atoms is calculated by means of QUANTUM CHEMISTRY methods and tabulated for each atom of the periodic table.
Official source: International Tables for Crystallography: Volume C
Unofficial but mostly used nowadays source: Crystallography group in Buffalo
http://harker.chem.buffalo.edu/group/ptable.html
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EXAMPLES of ATOMIC SCATTERING FACTORS*
Na atom
Ga atom
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STRUCTURE FACTOR
1
( ) ( )exp 2 ( )n
F hkl f i hx ky lzm m m mm
p=
= H STRUCTURE FACTOR
USING THE DEFINITION of ATOMIC SCATTERING FACTOR and the position of each atom in the unit cell, [xm ,ym ,zm ] we can rewrite the amplitude of scattering by the single unit cell as
THE SQUARE OF THE STRUCTURE FACTOR DEFINES THE INTENSITY OF THE REFLECTION with the indices h,k and l.
STRUCTURE FACTOR is an ACTUAL LINK BETWEEN CRYSTAL STRUCTURE (atomic positions xm, ym and zm) and INTENSITY OF X-ray DIFFRACTION
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A bit of terminology: real AND reciprocal space Real space Reciprocal space
Description of real crystal structure, i.e. distribution of electron density or atomic
positions
Distribution of diffraction intensity as a function of the
scattering vector
( ) r ( )A H
CRYSTAL STRUCTURE RECIPROCAL LATTICE
F1 F2
F3
F4
F5
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Investigation of crystal structures by means of X-ray diffraction technique
X-ray beam
Diffraction images
50 mm
Data analysis
Crystal structure
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The main goals of an X-ray diffraction experiment
A COLLECTION OF INFORMATION ABOUT RECIPROCAL SPACE
Locating positions of the diffraction maxima, i.e. reciprocal lattice points
Crystal lattice constants and symmetry
Reconstruction of the reciprocal lattice
Determination of the Bravais type of crystal lattice
Finding the orientation of lattice vectors, a*, b* and c*
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Physics
Determination of intensities of individual reflections
Analysing the SYMMETRY of RECIPROCAL SPACE
ASSIGNMENT OF THE SPACE GROUP OF INVESTIGATED CRYSTAL
STRUCTURE SOLUTION (determination or refinement of atomic positions in the unit cell)
The main goals of an X-ray diffraction experiment
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X-ray diffractometer
X-ray SOURCE(S)
Crystal holder
DETECTOR of X-rays
Goniometer with motors
Liquid nitrogen jet Observation
camera
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Spectra of the X-ray beam
Shortest wavelength
Shortest wavelength of the white X-ray beam (highest energy of an X-ray photon) is determined by the highest energy of electron hitting the target.
min
hc
eUl =
lmin ( Å ) = 12.39 / U (kV)
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Monochromatic X-ray beams The wavelength of the CHARACTERISTIC X-ray beam depends on the
material of the target and the electron shells involved in the transition
Anode type Radiation Wavelength, Å
Cu Cu, Ka
Energy, keV
Mo Mo, Ka
1.5406
Ag
Fe
0.7107
Ag, Ka 22.162 0.5477
Fe, Ka 6.402 1.9351
17.433
8.0423
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Diffraction in the monochromatic X-ray beam
The majority of modern X-ray diffraction techniques use a monochromatic X-ray beam (Dl / l ≈ 10-4 Å).
Which part of the reciprocal space is available from the X-ray diffraction pattern obtained from a STILL CRYSTAL???
The answer is given by the EWALD CONSTRUCTION
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1/λ k0
H
k1-k0 =H
Ewald sphere
X-ray beam, l 2θ
Detector
k1 k1
2θ
The wavelengths of the primary X-ray beam and the diffracted beam are the same, therefore |k0|=|k1|=1/l. Therefore the scattering vector H=k1-k0 always points to the surface of the sphere of radius 1/l with the center at the point –k0. This sphere is referred to as an Ewald sphere
CRYSTAL
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X-ray diffraction from a rotated crystal What happens if we rotate a crystal by a certain angle whilst
collecting an image from the detector?
1/λ
Detector
X-ray beam
Ewald sphere
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Rotation photographs (taken at single crystal diffractometer, rotation angle 1 degree)
a=b=c=3.8 Å a = b = g =90 deg a=10.2 Å b=15.4 Å c=18.3 Å
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Modern X-ray diffraction experiment
Taking the number of ROTATION PHOTOGRAPHS with very small step at different orientations of a crystal. Taking images frame by
frame
Reconstructing reciprocal space
Calculating distribution of intensities in the selected sections of the reciprocal space
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Reconstruction of reciprocal space: Example 1
a=37.05 b=8.69 c=20.7 Å a=90 b=95.97 g=90 deg
C10H10N2F6PClRu crystal (Guy Clarkson, Department of Chemistry, University of Warwick)
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Reciprocal space of a crystal: Example 2
a=b=c=3.8 Å a = b = g =90 deg
a*
b*
Na0.5Bi0.5TiO3 crystal (Ferroelectrics and crystallography group, Department of Physics, University of Warwick)
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Examples of reciprocal space reconstruction
Chernyshev, D., Bosak, A. European Synchrotron Radiation Facility
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Examples of DXS (BM01A @ ESRF)
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Results: diffuse scattering around 0 3 -2
0 3 -2
Resolution ~ 0.001 r.l.u
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Diffraction in the POLYCHROMATIC X-ray beam
The diffraction in the polychromatic beam was historically the first method of X-ray crystallography. Although it does not allow for the accurate quantitative studies (some recent exceptions are available) it can be preferential for simple task such as testing the quality of a crystal and defining the orientation of the crystallographic axes.
The diffraction in the polychromatic beam is usually referred to as Laue
method
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X-ray tube
White X-ray beam
Crystal
Photographic film
The schematic view of the experiment
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Ewald construction for the Laue method
1/λ
Detector
Any reciprocal lattice point within the LARGEST EWALD sphere (of radius 1/lmin contribute to the Laue pattern)
1/λmin
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Laue diffraction pattern
Laue diffraction pattern
λ1
λ2
λ4
λ3
Each Bragg reflection is diffracted at its own wavelength. Usually 2D detectors do not give the information about the wave length
therefore each spot reconstructs the direction of reciprocal space only
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Different Laue diffraction patterns
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Laue diffraction from protein crystals
John Helliwell, University of Manchester, UK
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Diffraction from the powder
A powder sample is composed of small, single crystalline, randomly oriented grains. Each grain has the same structure, i.e. the same lattice, space group and fractional positions of atoms in the unit cell. As a result each point of the reciprocal lattice is represented by a sphere. Reciprocal space of a powder is the set of concentric spheres
Powder diffraction is an important technique for the structure determination. The solution of a structure from
powder diffraction is known as Rietveld refinement
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Ewald construction for the powder diffraction
Ewald sphere
Primary beam
Reciprocal lattice point Sphere
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Typical powder diffraction pattern
Powder diffraction is one dimensional data representing the spherically averaged reciprocal lattice of a crystal. The position of each peak corresponds to the LENGTH of a reciprocal lattice vector.
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Splitting of the peak positions: example 1
a*=1 b*=1 a=90 deg
Cubic crystal system
a*=1.02 b*=1 a=90 deg
Tetragonal crystal system
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Splitting of the peak positions: example 2
a*=1 b*=1 a=90 deg
Cubic crystal system
a*=1 b*=1 a=89 deg
‘Rhombohedral’ crystal system
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Powder diffraction showing splitting of peaks
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Cubic to tetragonal (paraelectric to ferroelectric) phase transition in BaTiO3. The temperature of the phase transition is known as Curie temperature
{200} cubic
(200) tetragonal (020) tetragonal (002) tetragonal
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Change of the symmetry as a phase transition
High symmetry (cubic) phase
Lower symmetry (tetragonal) phase
{200} {210} {211}
(200) (020)
(002) (012) (021)
(210)
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Example 2: Following phase transitions
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Single crystal structure refinement
1
( ) ( )exp 2 ( )n
F hkl f i hx ky lzm m m mm
p=
= H
CRYSTAL STRUCTURE
NB! Remember that reflection intensities are 𝐼 ℎ𝑘𝑙 = 𝐹 ℎ𝑘𝑙 2
Additional factors to be taken into account: • Thermal motion (Debye-Waller factors) • Anomalous scattering • Structural disorder (Static Debye-Waller
factors) • Anharmonic motion
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Reliability (R) factor
CRYSTAL STRUCTURE
𝑅𝑤 = 𝑤ℎ𝑘𝑙 ∙ 𝐹𝑂𝐵𝑆
2 − 𝐹𝑆𝐼𝑀2 2
ℎ𝑘𝑙
𝑤ℎ𝑘𝑙 ∙ 𝐹𝑂𝐵𝑆2 2
ℎ𝑘𝑙
Weight of each reflection OBSERVED STRUCTURE FACTOR
SIMULATED STRUCTURE FACTOR
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Modern software for single crystal X-ray diffraction
Developed by George Sheldrick: University of Goettingen
38320 citations
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Modern software for single crystal X-ray diffraction
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Powder diffraction (Rietveld) refinement Determination and refinement of crystal structures using powder diffraction profiles is known as Rietveld refinement! It is named after Hugo Rietveld who developed the mathematical algorithms and prescribed the procedure of refinement.
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Rietveld refinement includes:
• Locating powder peaks • Indexing of reflections (assigning
hkl to each individual peak) (mind the peak overlap)
• Determination of lattice constants
• Deducing the shape of the peaks, separating overlapping profiles
• Refinement of peak shape parameters
• Refinement of atomic positions • Refinement of thermal
displacement parameters
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Modern software for Rietveld Refinement: TOPAS
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Modern software for Rietveld Refinement: FULLPROF