Title: Space Symmetry I
1Space Symmetry I
- Definition a crystal consists of atoms arranged
in a pattern that repeats periodically in 3-D. - note doesnt require (or acknowledge) surface.
- pattern can be 1 atom, groups of atoms, 1
molecule, groups of molecules. - Question In what form does NaCl exist?
2Space Symmetry I
- Definition a crystal consists of atoms arranged
in a pattern that repeats periodically in 3-D. - note doesnt require (or acknowledge) surface.
- pattern can be 1 atom, groups of atoms, 1
molecule, groups of molecules. - Question In what form does NaCl exist?
- As a crystal lattice a regular geometrical
arrangement of points or objects over an area or
space. - not necessarily ionic.
- A lattice is not a physical thing it is simply
an abstraction, a collection of points whereupon
real objects may be placed. F.A. Cotton
3Lattice Points
- As an analog of a 2-D crystal, look at an
infinitely large piece of wall paper, where the
pattern (which can be of any complexity) repeats
periodically in both dimensions. - Imagine that you are an infinitely small person
standing at a randomly chosen point on the
wallpaper. You examine your surroundings. - You are blindfolded and moved in a certain
distance along a straight line to a 2nd point.
You look around and cant tell that you have
moved. Where are you?
?
4Lattice Points
- As an analog of a 2-D crystal, look at an
infinitely large piece of wall paper, where the
pattern (which can be of any complexity) repeats
periodically in both dimensions. - Imagine that you are an infinitely small person
standing at a randomly chosen point on the
wallpaper. You examine your surroundings. - You are blindfolded and moved in a certain
distance along a straight line to a 2nd point.
You look around and cant tell that you have
moved. Where are you?
?
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5Lattice Points
- What happens if you are moved again an identical
distance still along that straight line? - the positions are each indistinguishable!
- What type of operation is this then? Symmetry!
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6Lattice Points
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- To aid in further discussion and calculations, it
will be convenient to choose some points and axes
of reference. - If we choose 1 point at random, then all points
identical with this point will constitute a set
of lattice points. - These points all have exactly the same
surroundings and are identical in position
relative to the repeating pattern. - NOMENCLATURE
- 1-D Row
- 2-D Net
- 3-D Lattice (or space lattice)
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7Lattice Points Unit Cell
- If we connect the lattice points by straight
lines, obtain 2-D parallelograms. - In 3-D this space is divided into
parallelepipeds. - Note that any one parallelogram is a template for
all of the rest. - Call this a UNIT CELL.
8Lattice Points Unit Cell
- If we connect the lattice points by straight
lines, obtain 2-D parallelograms. - In 3-D this space is divided into
parallelepipeds. - Note that any one parallelogram is a template for
all of the rest. - Call this a UNIT CELL.
- The choice of the initial lattice point could
have been anywhere. - If we know the exact atomic arrangement in one
unit cell, then we, by extension, can know the
arrangement of the whole crystal.
9Primitive Unit Cells
- The choice of a unit cell is not unique any
parallelogram whose edges connect lattice points
is a valid unit cell. So, infinite number of ways
of choosing a unit cell for a given structure. - Definition A unit cell with lattice points only
at the corners primitive.
10Centered Unit Cell
- It is permissible to have lattice points inside a
unit cell. - Definition A unit cell containing more than one
lattice point centered. - Well talk later about why you might want this.
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11Size and Shape of a Unit Cell
- May be specified by means of the lengths a, b c
of the three independent edges, and the three
angles, a, ß ? between the edges. - a is the angle between b c,
- ß is the angle between a c,
- ? is the angle between a b.
- The location of a point within a unit cell is
specified by three fractional coordinates x, y,
z. This point is located by starting at the
origin (0, 0, 0) and moving a distance xa along
the a axis, yb parallel to the b axis, and zc
parallel to the c axis.
This point is located at (0.5. 0.75, 0.6).
12Size and Shape of a Unit Cell
- If x, y or z 1, then you are all the way across
the unit cell. - If any are gt 1, then the point is in the next
unit cell. - e.g. (1.30, 0.25, 0.15) is identical to (0.30,
0.25, 0.15), since all unit cells are identical. - one of the advantages of fractional coordinates
is that 2 points are equivalent if the fractional
parts of their coordinates are equal. - caveat
- (-0.70, 0.25, 0.15) (0.30, 0.25, 0.15)
differ by 1
13Crystallographic Symmetry
- Our ultimate goal will be to consider 3-D arrays,
but it will be useful to consider 1-D and 2-D
arrays first. Most of the concepts applicable to
3-D can be illustrated more simply with 1-D and
2-D arrays. - The type of array we are concerned with is
obtained by repetition of some object or unit in
a regular way thoughout space. Our object, motif
- Weve defined symmetry operations as movements
after which no change could be detected in the
object it is indistinguishable. - Thus far, weve looked at the following E, Cn,
s, Sn, and i. - What do these have in common? At least one point
of the object is unmoved by the operation. - A complete symmetry classification scheme for
crystallography requires that we consider other
operations as well. Before we were dealing with
finite objects now with infinite arrays.
14Crystallographic Symmetry Operations
- Translation. Shifting a motif by a defined
distance in a certain direction, then doing this
again and again by the same distance and
direction. - This distance unit translation.
- Can be in 1-D, 2-D or 3-D (each with different
unit translation and direction) - ALL crystals possess translation.
15Crystallographic Symmetry Operations
- Translation. Shifting a motif by a defined
distance in a certain direction, then doing this
again and again by the same distance and
direction. - This distance unit translation.
- Can be in 1-D, 2-D or 3-D (each with different
unit translation and direction) - ALL crystals possess translation.
- Glide Plane. A combination of translation and
reflection. Operation is translation by one-half
unit dimension, followed by reflection in the
plane.
glide plane
16One Dimensional Space Groups
- A Space Group includes both point symmetry
elements and translation. - There are seven One Dimensional Space Groups.
- pxyz nomenclature
- p primitive (i.e. one lattice point per unit
cell). - x mirror plane - to axis of translation? yes
m no 1. - y mirror plane to axis of translation? yes
m - glide plane along axis of
translation? yes a -
no 1. - z Cn axis? n 1 n 2.
- p111 simplest only translation present.
- p1a1 includes glide plane.
17One Dimensional Space Groups
- pm11 translation and transverse reflection. Note
that second set of mirror planes are generated.
Often introduction of 1 set of symmetry elements
creates a second not equivalent to the first. - p1m1 translation with longitudinal reflection.
- p112 two-fold rotation axis (located below the
motif on the line of translation). The second C2
axis is explicitly introduced. If you had started
with it, the first would have arisen
automatically.
18One Dimensional Space Groups
- pma2 glide plane plus transverse reflection. C2
axis created automatically. - pmm2 translation with longitudinal and
transverse reflection. Just as in point groups,
the intersection of two mirrors generates a C2
axis.
19One Dimensional Space Groups
20One Dimensional Space Groups Examples
21One Dimensional Space Groups Examples
p1m1
22One Dimensional Space Groups Examples
p1m1
p111
23One Dimensional Space Groups Examples
p1m1
p111
p1a1
24One Dimensional Space Groups Examples
p1m1
p111
p112
p1a1
25One Dimensional Space Groups Examples
26One Dimensional Space Groups Examples
pm11
27One Dimensional Space Groups Examples
pm11
pma2
28One Dimensional Space Groups Examples
pm11
pma2
pmm2