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1 Massless fermion in Graphene Habib Rostami IPM December 18,2011

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Page 1: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

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Massless fermion in Graphene

Habib Rostami

IPM

December 18,2011

Page 2: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

Outline

allotropes of Carbon

Two dimensional lattice stability

Electronic structure of Graphene

Experimental evidences for massless

fermions in graphene

2

Page 3: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

Carbon

3 http://en.citizendium.org/wiki/life

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The allotropes of Carbon

4 http://chemistry.tutorvista.com/inorganic-chemistry/allotropes-of-carbon.html

Page 5: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

Diamond And Graphite

5 http://en.wikipedia.org/wiki/File:Diamond_and_graphite2.jpg

Page 6: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

New allotropes of Carbon

6

Fullerene

Harold Kroto, et al

1986

Carbon nanotube

Sumio Iijima

1991

Graphene

2004

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Graphene for the first time!!!

Page 8: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

Graphene for the first time

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Page 9: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

Graphene

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Page 10: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

2D!

10 Peierls(1934), Landau(1937) ,Mermin&Wagner(1966)

In harmonic approximation

D=2

Logarithmic Divergence

Page 11: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

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Anharmonic terms

Statistical Mechanics of Membranes and Surfaces by: David Nelson, Steven Weinberg, T Piran

Page 12: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

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Transmission Electron Microscope image

Ripple in Graphene

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Electron diffraction pattern

Page 14: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

The fabrication of Graphene

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Mechanical cleavage

silicon carbide is heated up to 1100 ◦C

Epitaxial growth on metal substrates

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C:1s2 2s2 2p2 →1s2 2s1 2p3

→(two)1s2 +(three)sp2 + (one)pz

1-S. Thompson and J. Staley. Orbitals and Molecular Representation 2-Jason E. Hill’s presentation

Carbon atoms in Graphene

Page 16: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

σ-bond and π-bond

16 McMurray and Fay. Chemistry 4th ed., Prentice-Hall, 2004.

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Tight-Binding Model

t≈3eV

arXiv:1110.6557v1, Daniel R. Cooper,2011 ,Experimental review of graphene

Page 18: Massless fermion in Graphenephysics.ipm.ac.ir/courses/pdfseminar1/rostami1.pdf15 C:1s2 22s 22p2 →1s 2s1 2p3 →(two)1s2 +(three)sp2 + (one)pz 1-S. Thompson and J. Staley. Orbitals

Tight-Binding Model

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Sublattice=Pseudospin

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Tight-Binding Model

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Massless Quasiparticle

Dirac Cone

Each state is 4-fold degenerate, 2 for spin and 2 for valley

The electronic properties of graphene, REVIEWS OF MODERN PHYSICS, 81,2009

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What we expect?

21

Linear Dispersion relation

New Landau levels

Cyclotron mass

Chirality and Kelin tunneling

Anomalous QHE

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Linear Dispersion relation

22 Bostwick, A., T. Ohta, T. Seyller, K. Horn, and E. Rotenberg,2007, Nature Physics 3(1), 36.

Angle-resolved photoemission spectroscopy (ARPES)

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The Landau levels of Massless particles

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24 http://en.wikipedia.org/wiki/Scanning_tunneling_microscope

STM

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The Landau level Massless Dirac particle

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Is Pseudospin a real parameter?

Are quasiparticles of Graphene Chiral?

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30 The electronic properties of graphene, REVIEWS OF MODERN PHYSICS, 81,2009

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Two dimensional electron gas

QUANTUM THEORY OF THE ELECTRON LIQUID By:Giuliani and Vignale

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Two dimensional electron gas

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Integer Quantum Hall effect

35

arXiv:1110.6557v1, Daniel R. Cooper,2011 ,Experimental review of graphene

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arXiv:1110.6557v1, Daniel R. Cooper,2011 ,Experimental review of graphene

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Interactions and disorders can destroy

our massless fermin

for example:

39

Interactions and disorders

Dirac charge dynamics in graphene by infrared spectroscopy nature physics, vol 4 ,2008

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So that they are massless fermion

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Thanks for your attention