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    Graphene

    Rachel WootenDepartment of Physics

    Solid State Physics II

    March 6, 2008

    Taught by Professor Dagotto

    [email protected]

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    Outline

    What is graphene?

    How it is made

    Properties

    Electronic & physical properties

    Relativistic charge carriers

    Anomalous quantum Hall effect

    Future Applications

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    2-dimensionalhexagonal lattice of

    carbon

    sp2 hybridized carbon

    atoms Basis for C-60 (bucky

    balls), nanotubes, and

    graphite

    Among strongestbonds in nature

    What is graphene?

    A. K. Geim & K. S. Novoselov. The rise of graphene. Nature Materials Vol 6183-191 (March 2007)

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    A Two dimensional crystal

    In the 1930s, Landau and Peierls (and Mermin, later)showedthermodynamics prevented 2-d crystals in free state.

    Melting temperature of thin films decreases rapidly withtemperature -> monolayers generally unstable.

    In 2004, experimental discovery of graphene- high quality 2-dcrystals

    Possibly, 3-d rippling stabilizes crystal

    http://www.nature.com/nmat/journal/v6/n11/fig_tab/nmat2011_F1.html#figure-title

    Representation of

    rippling in

    graphene. Red

    arrows are

    ~800nm long.

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    How to make graphene

    Strangely cheap and easy.

    Either draw with a piece of graphite, or

    repeatedly peel with Scotch tape Place samples on specific thickness of Silicon

    wafer. The wrong thickness of silicon leaves

    graphene invisible. Graphene visible through feeble interference

    effect. Different thicknesses are differentcolors.

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    Samples of graphenea) Graphite films

    visualized through

    atomic forcemicroscopy.

    b) Transmissionelectron

    microscopy image

    c) Scanning

    electron

    microscope imageof graphene.

    A. K. Geim & K. S. Novoselov. The rise of graphene. Nature Materials Vol 6183-191 (March 2007)

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    Electrons in graphene

    Electrons in p-orbitals above andbelow plane

    p-orbitals becomeconjugated acrossthe plane

    Electrons free to

    move across plane indelocalized orbitals

    Extremely high

    tensile strength

    http://en.wikipedia.org/wiki/Aromaticity

    -Graphene and graphite are great

    conductors along the planes.

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    Properties: charge carriers

    Samples are excellent- graphene is ambipolar:charge carrier concentration continuously tunable

    from electrons to holes in high concentrations

    A. K. Geim & K. S. Novoselov. The rise of graphene. Nature Materials Vol 6183-191 (March 2007)

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    Relativistic charge carriers

    Linear dispersion relation- charge

    carriers behave like massless Dirac

    fermions with an effective speed of light

    c*~106

    . (But cyclotron mass is nonzero.) Relativistic behavior comes from

    interaction with lattice potential of

    graphene, not from carriers moving near

    speed of light.

    Behavior ONLY present in monolayer

    graphene; disappears with 2 or more

    layers.K. S. Novoselov, A. K. Geim, S. V. Morozov, D. Jiang, M. I. Katsnelson, I. V. Grigorieva, S. V.Dubonos, & A. A. Firsov. Two-dimensional gas of massless Dirac fermions in graphene.

    ature, 438 197-200 (2005)

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    Anomalous quantum Hall effect

    Classical quantum Hall effect. Apply B field and current. Charges build up on opposite sides

    of sample parallel to current.

    Measure voltage: + and - carriers create opposite Hall voltages.

    Quantum Hall effect Classical Hall effect with voltage differences = integer times

    e2/h

    http://www.eeel.nist.gov/812/effe.htm

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    Anomalous quantum Hall effect

    Fractional Quantum Hall effect

    Quantum Hall effect times rational fractions.

    Not completely understood. Graphene shows integer QHE shifted by 1/2

    integer

    Non-zero conductivity as charge carrierdentsity -> zero.

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    Hall

    conductivity

    xy (red) andresistivity xyvs. carrier

    concentration.

    Inset: xy in 2-layer graphite.

    Half-integer

    QHE unique to

    monolayer.

    *Note non-zero conductivity as carrier concentrations approach zero.K. S. Novoselov, A. K. Geim, S. V. Morozov, D. Jiang, M. I. Katsnelson, I. V. Grigorieva, S. V.Dubonos, & A. A. Firsov. Two-dimensional gas of massless Dirac fermions in graphene.

    ature, 438 197-200 (2005)

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    Possible Applications

    High carrier mobility even at highest electric-field-induced concentrations, largely unaffected bydoping= ballistic electron transport over < mdistances at 300K

    May lead to ballistic room-temperature transistors.

    GaTech group made proof of concept transistor- leakselectrons, but its a start.

    Energy gap controlled by width of graphene strip.

    Must be only 10s of nm wide for reasonable gap.

    Etching still difficult consistently and random edgeconfiguration causes scattering.

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    Even more applications?

    Very high tensile strength

    Replacement of nanotubes for cheapness in

    some applications: composite materials andbatteries for improved conductivity

    Hydrogen storage

    Graphene based quantum computation?Low spin-orbit coupling-> graphene may beideal as a q-bit.

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    In Conclusion

    Graphene is a novel material with veryunusual properties

    Easy to make in lab; may prove easy andeconomical to manufacture (unknown).

    Broad range of applications for future

    research. Variety of possible practical applications.

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    Resources 1. A. K. Geim & K. S. Novoselov. The rise of graphene. Nature Materials Vol 6183-191 (March

    2007)

    2. N. D. Mermin. Crystalline Order in Two Dimensions. Phys. Rev. 176, 1 250-253

    3. H. W. Kroto, J. R. Heath, S. C. OBrien, R. F. Curl & R. E. Smalley. C60: Buckminsterfullerene.Nature 318, 162-163 (1985).

    4. Sumio Iijima. Helical microtubules of graphitic carbon. Nature 354, 56-58 (1991).

    5. P. R. Wallace. The band theory of graphite. Phys. Rev. 71, 622-634 (1947).

    6. J. C. Slonczewski & P. R. Weiss. Band structure of graphite. Phys. Rev. 109, 272-279 (1958).

    7. A. Fasolino, J. H. Los & M. I. Katsnelson. Intrinsic ripples in graphene. Nature Materials 6,858-861 (2007)

    8. K. S. Novoselov, et al. Electric field effect in atomically thin carbon films.Science306, 666-669 (2004).

    9. K. S. Novoselov, A. K. Geim, S. V. Morozov, D. Jiang, M. I. Katsnelson, I. V. Grigorieva, S. V.Dubonos, & A. A. Firsov. Two-dimensional gas of massless Dirac fermions in graphene.Nature, 438

    197-200 (2005) 10. Adriaan M. J. Schakel. Relativistic quantum Hall effect. Phys. Rev. D 43, 4 1428-1431 (1991)

    11. J. Hass, R. Feng, T. Li, X. Li, Z. Zong, W. A. de Heer, P. N. First & E. H. Conrad. Highlyordered graphene for two dimensional electroncs. Applied Physics Letters 89, (2006)

    12. Prachi Patel-Predd. Ultrastrong paper from graphene. July 25, 2007.http://www.technologyreview.com/Nanotech/19097/

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    End

    http://en.wikipedia.org/wiki/Graphite