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 Submitted to –
Mr.Gyanrao
Dhote
 Submitted by -
Kamini Malviya
A unit cell of the crystal is an
imaginary parallel-sided region from
which the entire crystal can be built
up.
Usually the smallest unit cell
which exhibits the greatest
symmetry is chosen. If repeated
(translated) in 3 dimensions, the
entire crystal is recreated.
•The simplest repeating unit in a crystal is
called a unit cell.
•Opposite faces of a unit cell are parallel.
•The edge of the unit cell connects equivalent
points.
•Not unique. There can be several unit cells of
a crystal.
•The smallest possible unit cell is called
primitive unit cell of a particular crystal
structure.
•A primitive unit cell whose symmetry matches
the lattice symmetry is called Wigner-Seitz
cell.
The Unit Cell Concept
•Each unit cell is defined in terms of lattice points.
•Lattice point not necessarily at an atomic site.
• For each crystal structure, a conventional unit
cell, is chosen to make the lattice as symmetric as
possible. However, the conventional unit cell is not
always the primitive unit cell.
•A crystal's structure and symmetry play a role in
determining many of its properties, such as
cleavage (tendency to split along certain planes
with smooth surfaces), electronic band structure
Symmetry elements: Four 3-fold
rotation axes along cube diagonals
a = b = c
 =  =  = 90o
3 Bravais lattices
Only one Bravais lattice
Symmetry element:
One 6-fold rotation
axis
a = b  c
= 120o
 =  = 90o
Symmetry element: One 4-
fold rotation axis
a = b  c
=  =  = 90o
Two Bravais
lattices
One Bravais lattice
Symmetry element: One
3-fold rotation axis
a = b  c
= 120o
 =  = 90o
Four Bravais lattices
Symmetry element: Three mutually
perpendicular 2-fold rotation axes
a  b  c
 =  =  = 90o
Two Bravais lattices
Symmetry element: One 2-fold rotation
axis
a  b  c
 =  = 90o,   90o
One Bravais lattice
Symmetry element:
None
a  b  c
      90o
CRYSTAL STRUCTURE

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CRYSTAL STRUCTURE

  • 1.
  • 2.  Submitted to – Mr.Gyanrao Dhote  Submitted by - Kamini Malviya
  • 3.
  • 4.
  • 5. A unit cell of the crystal is an imaginary parallel-sided region from which the entire crystal can be built up. Usually the smallest unit cell which exhibits the greatest symmetry is chosen. If repeated (translated) in 3 dimensions, the entire crystal is recreated.
  • 6. •The simplest repeating unit in a crystal is called a unit cell. •Opposite faces of a unit cell are parallel. •The edge of the unit cell connects equivalent points. •Not unique. There can be several unit cells of a crystal. •The smallest possible unit cell is called primitive unit cell of a particular crystal structure. •A primitive unit cell whose symmetry matches the lattice symmetry is called Wigner-Seitz cell. The Unit Cell Concept
  • 7. •Each unit cell is defined in terms of lattice points. •Lattice point not necessarily at an atomic site. • For each crystal structure, a conventional unit cell, is chosen to make the lattice as symmetric as possible. However, the conventional unit cell is not always the primitive unit cell. •A crystal's structure and symmetry play a role in determining many of its properties, such as cleavage (tendency to split along certain planes with smooth surfaces), electronic band structure
  • 8.
  • 9. Symmetry elements: Four 3-fold rotation axes along cube diagonals a = b = c  =  =  = 90o 3 Bravais lattices
  • 10. Only one Bravais lattice Symmetry element: One 6-fold rotation axis a = b  c = 120o  =  = 90o
  • 11. Symmetry element: One 4- fold rotation axis a = b  c =  =  = 90o Two Bravais lattices
  • 12. One Bravais lattice Symmetry element: One 3-fold rotation axis a = b  c = 120o  =  = 90o
  • 13. Four Bravais lattices Symmetry element: Three mutually perpendicular 2-fold rotation axes a  b  c  =  =  = 90o
  • 14. Two Bravais lattices Symmetry element: One 2-fold rotation axis a  b  c  =  = 90o,   90o
  • 15. One Bravais lattice Symmetry element: None a  b  c       90o