Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

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Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang Lecture 2 Fermi Gas

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Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang. Lecture 2 Fermi Gas. Enrico Fermi 1901 - 1954. Paul Dirac 1902 - 1984. Band Theory of Metals. Start with isolated Sodium Atom. Ionisation Energy of Sodium 5.14 eV. Band Theory of Metals. - PowerPoint PPT Presentation

Transcript of Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Page 1: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Graduate Lecture Series29 June – 3 July, 2009

Prof Ngee-Pong Chang

Lecture 2

Fermi Gas

Page 2: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Enrico Fermi

1901 - 1954

Paul Dirac

1902 - 1984

Page 3: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Ionisation Energy of Sodium 5.14 eV

Band Theory of Metals

Start with

isolated Sodium Atom

Page 4: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Ionisation Energy of Sodium 5.14 eV

Band Theory of Metals

Page 5: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Band Theory of Metals

Page 6: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Band Theory of Metals

Splitting of 3s level with 2 Sodium atoms

Bring two

Sodium Atoms

together

Page 7: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Band Theory of Metals

Splitting of 3s level with 6 Sodium atoms

Bring six

Sodium Atoms

together

Page 8: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Band Theory of Metals

Splitting of 3s levels with Sodium atoms in crystalline solid

Page 9: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Band Theory of Metals

Page 10: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Fermi-Dirac Distribution

electrons

holes

Page 11: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Probability of Occupancy

1.0

0.0

T=0

T > 0

Page 12: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Probability of Occupancy

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Energy in

units

Filling up the Fermi Sea

In One Dimensional Box

10

20

30

²F

Page 14: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

1-Dimensional Box

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1-Dimensional Fermi Gas

Sum Over Spins

Page 16: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

1-Dimensional Fermi Gas

Single Spin Orientation

Fermi Surface dependence on

number of electrons

Page 17: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

2-Dimensional Fermi Gas

Single Spin Orientation

Fermi Surface dependence on

number of electrons

Page 18: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

3-Dimensional Fermi Gas

Single Spin Orientation

Fermi Surface dependence on

number of electrons

Page 19: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang
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1-Dimensional Fermi Gas

Single Spin Orientation

Total Energy

Page 21: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

2-Dimensional Fermi Gas

Single Spin Orientation

Total Energy

Page 22: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

3-Dimensional Fermi Gas

Single Spin Orientation

Total Energy

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Page 24: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

3-Dimensional Density of States

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2-Dimensional Density of States

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http://upload.wikimedia.org/wikipedia/en/c/c5/DOS_multdim.jpg

Page 27: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

3-Dimensional Fermi Gas

Density of States

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2-Dimensional Fermi GasDensity of

States

Page 29: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

1-Dimensional Fermi GasDensity of

States

Page 30: Graduate Lecture Series 29 June – 3 July, 2009 Prof Ngee-Pong Chang

Conduction Band

Valence Band

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Woodward Yang harvard lecture notes

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CBO =conduction band offset

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2-Dimensional Density of States

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Quantum Wire

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http://boulder.research.yale.edu/Boulder-2005/Lectures/Matveev/Boulder%20lecture.pdf

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A graphene nanoribbon field-effect transistor (GNRFET). Here contacts A and B are at two different Fermi levels EF1 and . EF2

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Ballistic Conductor

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i

i’t’

t

Landauer formula

1927 - 1999

Conductance

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µ

Gas Pressure on the Wall

A cos θ

v δ t

A

θ

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Pressure due to

Non-Relativistic Degenerate Fermi Gas

Equation of state for Fermi Gas

since at T = 0

We have

for a metal

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White dwarf as seen by Hubble Space Telescope

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What's Inside a White Dwarf?

To say that white dwarfs are strange is an understatement. An earth-sized white dwarf has a density of

1 x 109 kg/m3.

In comparison, the earth itself has an average density of only 5.4 x 103 kg/m3.

That means a white dwarf is 200,000 times as dense!