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Lecture 2
Crystal Structure 1
MSEG 608
September 2, 2021
Prof. LaShanda Korley ([email protected])
Prof. Xi Wang ([email protected])
Material categories
wikipedia
• Crystalline materials •
have long range
order (atoms,
molecules, ions, etc)
– Salt, gemstones,
snowflakes
Polycrystalline • Amorphous
materials have materials are
pockets of order disordered
– Ice, metals,
ceramics
(usually)
– Plastics, wax,
frequently
polymers
Crystals
• Google “nature crystals”
Polycrystalline
Polycrystalline monocrystalline
Silicon
wikipedia
Diamond
http://www.superabrasivespowder.com/products/polypolycrystalline-diamond-powder.html
Amorphous solids
• Amorphous solid: no order on any
“significant” length scale
• Blurry line between amorphous solids and
nanocrystalline materials
http://www.sunflower-solar.com/index.php?act=content&scheduler_id=429
Amorphous
• Glasses, liquids, colloids, gels, etc
• Polymers tend to easily form glassy states
• Glasses are an amorphous state
– SiO2 glass
• Usually contents other components
– fused silica/fused quartz
Amorphous semiconductors
• Silicon, germanium
– Primarily for solar cells
• Chalcogenides
– AsS, GeS, GeSbTe, AgInSbTe
– Infrared detectors, modulatle IR
optics, IR fibers, rewritable disks
• More scattering
• Less efficient
• Still carry current
• Cheaper, easier to process
“The deepest and most interesting
unsolved problem in solid state theory
is probably the theory of the nature of
glass and the glass transition. The
solution of the (...) important and
puzzling glass problem may also have
a substantial intellectual spin-off.
Whether or not it will help make
better glass is questionable.”
P.W. Anderson, Science (1995)
Crystal Structures
• “Easy” modelling
• Historically
Uvarovite
– External appearance
• Today
– Internal structure
• Flat facets
• Fixed angles between facets
• Experience: Crystal formation
(crystallization) is from liquid to
solid.
• Modelling: Something internal?
Early study
• Snowflakes: always showed perfect
six-cornered symmetry and never
showed five or seven corners
• Material structure modeling since
17th century
• Particle packings
http://www.xtal.iqfr.csic.es/Cristalografia/index-en.html
Bravais Lattices
• concluded that the crystals
were made by the ordered
stacking of small bricks, or
unit cells, all of them
identical.
René Just Haüy (1743-1822)
• In 1848 the French physicist Auguste
Bravais discovered that in the threedimensional space, periodic repetitions
by translation can only be made in 14
different modes (the so-called 14 Bravais
lattices), as they must to be compatible
with the 32 crystal classes.
Auguste Bravais (1811-1863)
http://www.xtal.iqfr.csic.es/Cristalografia/index-en.html
Crystal structures
• 50 years later, the 14 Bravais lattices and the 32 crystal
classes were the limitations used to independently deduce
the 230 space groups, which are the 230 possible ways to
restrict distributions of repetitive structural units of the
crystals (atoms, ions and molecules).
Mercury
• Cif files
• https://www.ccdc.cam.ac.uk/solutions/csdsystem/components/mercury/
• http://www.crystallography.net/cod/index.ph
p
Key Concepts
•
•
•
•
Lattice
Basis
Primitive cell
Unit cell
Lattice
• A periodical set of mathematical points
𝐫′ = 𝐫 + 𝑙𝐚1 + 𝑚𝐚2 + 𝑛𝐚3
l, m, n are arbitrary integers; 𝐚1 , 𝐚2 , 𝐚3 are primitive vectors
• The environment of any given point is equivalent to
the environment of any other given point.
• Primitive lattice vectors
– Any two points can
be translated
– Smallest
𝐚1 ⋅ (𝐚2 × 𝐚3 ) 3D
𝐚1 × 𝐚2 2D
Basis
• Infinite repetition of identical groups of atoms
• Crystal structure = Basis + Lattice
– Number of atoms in a basis: >=1
– Position of an atom j r j  x j a1  y j a 2  z j a3
0<= xj, yj, zj <=1
Primitive cell
• The volume/area defined by primitive vectors
– Many ways
– One lattice point per primitive cell
• Number of atoms in a primitive cell is always the
same for a given crystal structure
– Minimum number of atoms among basis
• Wigner-Seitz cell
Unit cell
• Conventional cells
– Often a nonprimitive cell
– A more obvious relation with the point symmetry
operations
– 2D
Unit cell
• Conventional cells
– Often a nonprimitive cell
– A more obvious relation with the point symmetry
operations
– 3D
sc
bcc
Fcc
Volume
a3
a3
a3
Lattice points per cell
1
2
4
Volume, primitive cell
a3
a3/2
a3/4
Number of nearest neighbors
6
8
12
The fourteen (3D) Bravais Lattices