Diffraction Flashcards

1
Q

How diffraction pattern spacing relates to the slit separation

A

x = slit spacing
1/x is proportional to spacing between diffraction spots

The orientation is retained e.g. horizontal slits make horizontal spots

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2
Q

Indexing diffraction spots

A

in 3D:

e.g. spot labelled 111 will be from (111) family of planes

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3
Q

How the angle between non-orthogonal axes changes through diffraction

A

The angle between the diffraction spots is now the complement of the angle between the original axes

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4
Q

Magnification with a lens

A

1/f = 1/u + 1/v

f = focal length
u = distance between object and lens
v = distance between lens and image
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5
Q

What limits the size of the smallest feature you can image

A

The wavelength of light used but be approximately equal to the size of the smallest feature

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6
Q

Abbe’s theorem

A

At least 2 beams must enter a lens to image a grating

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7
Q

Methods of generating x-rays

A
  1. Heat a filament so that electrons are thermionically emitted
  2. Accelerate the electrons through a large potential difference
  3. Focus the accelerated electrons on a target
  4. 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 —
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8
Q

Continuous spectrum

A

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.

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9
Q

Characteristic peaks

A

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

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10
Q

Why Kalpha1 peak has a greater intensity than the Kalpha2 peak

A

There are double the electrons in LIII than in LII

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11
Q

Foils used to absorb certain wavelengths

A

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

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12
Q

Bragg reflection

A

Arise from constructive interference between X-rays scattered by atoms within a crystal

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13
Q

Powder diffraction

A

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

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14
Q

Debye-Scherrer camera

A

Strips of film in a circle about the sample.

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15
Q

Systematic absences

A

Occur when planes of atoms reflects beams that are in antiphase with each other –> destructive interference

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16
Q

Atomic scattering factor (f)

A

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

17
Q

Structure factor (F)

A

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

18
Q

Intensity of a scattered wave

A

Intensity is proportional to the square of the magnitude of the structure factor i.e. structure factor * its complex conjugate

19
Q

Using the structure factor in non-primitive systems

A

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)

20
Q

Why intensity is proportional to multiplicity for powder refraction

A

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

21
Q

How to index planes from diffraction pattern

A

2x = 2theta

Columns:

  1. 2x
  2. x
  3. sin(x)
  4. (sin(x))^2
  5. (sin(x))^2 / (sin(x1))^2 (may need to be multiplied by a factor to find 6.)
  6. h^2 + k^2 + l^2
  7. hkl
22
Q

How to find motif from diffraction pattern

A

Calculate structure factors for some peaks based on possible motifs.
Compare to the observed intensities

23
Q

How to calculate lattice parameters

A

Most accurate value from a single measurement is to use the highest diffraction angle

24
Q

Systematic absences for hexagonal

A

h-k = a multiple of 3