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Condensed Condensed matter matter Forms of matter as we know: How do atoms condense when they want to minimize How do atoms condense when they want to minimize energy? energy?

Condensed matter

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How do atoms condense when they want to minimize energy?. Forms of matter as we know:. Condensed matter. Crystal structures in materials. A unique arrangement of atoms that fill space in 3D (Real-life) when repeating (Translational Property). - PowerPoint PPT Presentation

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Page 1: Condensed matter

Condensed matterCondensed matter

Forms of matter as we know:

How do atoms condense when they want to minimize energy?How do atoms condense when they want to minimize energy?

Page 2: Condensed matter

Crystal structures in materialsCrystal structures in materials

A unique arrangement of atoms that fill space in 3D (Real-life) when repeating (Translational Property)

Everytime a unit cell is translated, it must be forming the entire lattice.

2D BCC 2D FCC

Page 3: Condensed matter

Is everything always in a crystalline order?Is everything always in a crystalline order?

Amorphization under electron bombardment in TEM

Page 4: Condensed matter

Glassy silica (from wikipedia)Glassy silica (from wikipedia)

Extremely short Extremely short range orderrange order

Nematic liquid crystal (orientational long range order)Nematic liquid crystal (orientational long range order)

Short range order Short range order in 2Din 2D

Page 5: Condensed matter

In 3D, there are seven types of crystal systems that make up 14 Bravais LatticesIn 3D, there are seven types of crystal systems that make up 14 Bravais Lattices

Triclinic, monoclinic, orthorhombic, tetragonal, rhombohedral, hexagonal and cubic

Translation vector = r T = r + u1a1 + u2 a2 + u3a3

r

X u1

X u2

X u3

Page 6: Condensed matter

The 14 Bravais lattices and their The 14 Bravais lattices and their unit cell characteristicsunit cell characteristics. .

Page 7: Condensed matter

The Wigner-Seitz Cell can also be a unit cell

Wigner-Seitz cell for sımple cubic in 3DWigner-Seitz cell for sımple cubic in 3D

Select a lattice point and draw construction lines to the nearest neighbouring points

Draw lines that perpendicularly bisect the construction lines

The smallest enclosed area represents the Wigner-Seitz cell. Here shown in orange.

Page 8: Condensed matter

We often deal with diffraction data of crystals. A real crystal can be expressed in reciprocal space (space-1)

Unit cell in real space Unit cell in reciprocal space

ab

1/a

1/b

No XNo X

interplanar distanceinterplanar distance

Page 9: Condensed matter

Why deal with the reciprocal lattice?Why deal with the reciprocal lattice?

-Easy to deal with points rather than planes.Easy to deal with points rather than planes.

-Every point represents a set of planes (a period that exists in your crystal).Every point represents a set of planes (a period that exists in your crystal).

-Diffraction experiments yield the reciprocal lattice (It is the Fourier transform Diffraction experiments yield the reciprocal lattice (It is the Fourier transform of a crystal – Believe it or not but nature takes the Fourier transform of your of a crystal – Believe it or not but nature takes the Fourier transform of your sample when carrying out, for instance, electron diffraction experiments in sample when carrying out, for instance, electron diffraction experiments in TEM or XRD).TEM or XRD).

-Very useful when talking about electrons in a crystal (coming soon).Very useful when talking about electrons in a crystal (coming soon).

Fourier Fourier TransformTransform

Page 10: Condensed matter

nnλλ = 2dsin = 2dsinθθ

Bragg’s equation:Bragg’s equation:

Diffracted waves have to be in phase! (To see a “net reflected” wave)

Page 11: Condensed matter

A crystal can be thought of being a periodic function in a given space.

What is meant by this?

n(r+T) = n(r)

Volume of the unit cell

Area of parallelogram

Page 12: Condensed matter

Primitive unit cells needed for the reciprocal primitive vectors

xy

z

xza

zya

yxa

21

3

21

2

21

1

a

a

a

zyxa

zyxa

zyxa

a

a

a

21

3

21

2

21

1

FCC primitive cellFCC primitive cell

BCC primitive cellBCC primitive cell

Page 13: Condensed matter

From International Union of CRYSTALLOGRAPHY (IUC) 

2.1 Definition Let a, b, c be the basic vectors defining the unit cell of the direct lattice. The basic vectors of the reciprocal lattice are defined by:    

“The modulus of a* is equal to the ratio of the area of the face OBCG opposite to a to the volume of the cell built on the three vectors a, b, c. Referring to Figure below, we may write”:

Page 14: Condensed matter

Again, why did we bother with the reciprocal lattice?Again, why did we bother with the reciprocal lattice?

Page 15: Condensed matter

Some examples to sets of planes in a real 2D lattice.

Page 16: Condensed matter

TEM image and electron diffraction pattern from a piezoelectric TEM image and electron diffraction pattern from a piezoelectric thin film. How to guess any secondary formations in the structure thin film. How to guess any secondary formations in the structure that might detoriate or enhance your material?that might detoriate or enhance your material?

Structural interpretation of a high-k layer grown on Si. Note the dislocations at the interface that form as a result of ‘lattice misfit’.

Page 17: Condensed matter

Matching of epitaxy of semiconductor layers with misfit.Matching of epitaxy of semiconductor layers with misfit.

Page 18: Condensed matter

An electron propagating in a crystal with wavelength a (k = 2π/λ)

a: lattice constant

Wave vector: Commonly used in discussing energies of electrons

k

Larger the k, higher the energy of the electron (inverse of wavelength is quite convenient when representing energies)

Page 19: Condensed matter