Diffraction Flashcards
How diffraction pattern spacing relates to the slit separation
x = slit spacing
1/x is proportional to spacing between diffraction spots
The orientation is retained e.g. horizontal slits make horizontal spots
Indexing diffraction spots
in 3D:
e.g. spot labelled 111 will be from (111) family of planes
How the angle between non-orthogonal axes changes through diffraction
The angle between the diffraction spots is now the complement of the angle between the original axes
Magnification with a lens
1/f = 1/u + 1/v
f = focal length u = distance between object and lens v = distance between lens and image
What limits the size of the smallest feature you can image
The wavelength of light used but be approximately equal to the size of the smallest feature
Abbe’s theorem
At least 2 beams must enter a lens to image a grating
Methods of generating x-rays
- Heat a filament so that electrons are thermionically emitted
- Accelerate the electrons through a large potential difference
- Focus the accelerated electrons on a target
- As the electrons hit the target, they decelerate. They lose energy by heating the target, emitting a photon or by exciting atoms in the target. Excited atoms will then emit a characteristic photon.
- – The target must be cooled as it heats up rapidly —
Continuous spectrum
When electrons hit the target, they emit photons as they decelerate. The only wavelengths not present in the continuous spectrum are those that correspond to a greater energy than the electrons were accelerated to.
If you want to use the continuous spectrum, use an element with a high atomic number as intensity is proportional to atomic number.
Characteristic peaks
Bombarding electrons ‘knock’ electrons out of atoms in the target or excite these atoms.
Electrons in these atoms return to lower energy levels and emit photons corresponding to the energy difference between their original and final energy levels.
Characteristic peaks have a greater intensity than the continuous spectrum
Why Kalpha1 peak has a greater intensity than the Kalpha2 peak
There are double the electrons in LIII than in LII
Foils used to absorb certain wavelengths
Use thin foils with absorption edges
Where the absorption is high, there’s a large probability of photons and electrons combining to create a photo-electron.
Where absorption decreases rapidly is where the energy is too low to create a photo-electron
Bragg reflection
Arise from constructive interference between X-rays scattered by atoms within a crystal
Powder diffraction
Powder of many crystals in compacted into a polycrystalline block
Each grain is in a random orientation
Produce Debye-Scherrer cones since 2theta can be in any orientation now
On film, the cones are circles made of many individual diffraction spots
Small d-spacing can lead to back reflections as 2theta is so large
Debye-Scherrer camera
Strips of film in a circle about the sample.
Systematic absences
Occur when planes of atoms reflects beams that are in antiphase with each other –> destructive interference
Atomic scattering factor (f)
Wave scattering from an individual atom
For a direct beam, f is maximal and is equal to the number of electrons per ion/atom in the sample.
(atomic number for an atom)
As the angle of scatter increases, f decreases
Structure factor (F)
Wave resulting from scattering from multiple atoms
The sum of all the atomic scattering factors taking into account their magnitudes and relative phase factors
F gives the amplitude of the resultant scattered wave
Intensity of a scattered wave
Intensity is proportional to the square of the magnitude of the structure factor i.e. structure factor * its complex conjugate
Using the structure factor in non-primitive systems
Split the structure factor into the contribution from the lattice and the motif
Multiply the structure factor of the lattice (has no atomic scattering factor) by the structure factor of the motif (with atomic scattering factors)
Why intensity is proportional to multiplicity for powder refraction
Number of individual crystals within a polycrystalline block that are in the correct orientation to cause diffraction is proportional to the multiplicity of the family of diffraction planes.
So, intensity is proportional to multiplicity
IN NON-CUBIC SYSTEMS, multiplicity decrease because e.g. a=b not equal to c
How to index planes from diffraction pattern
2x = 2theta
Columns:
- 2x
- x
- sin(x)
- (sin(x))^2
- (sin(x))^2 / (sin(x1))^2 (may need to be multiplied by a factor to find 6.)
- h^2 + k^2 + l^2
- hkl
How to find motif from diffraction pattern
Calculate structure factors for some peaks based on possible motifs.
Compare to the observed intensities
How to calculate lattice parameters
Most accurate value from a single measurement is to use the highest diffraction angle
Systematic absences for hexagonal
h-k = a multiple of 3