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    Department of Materials Science and Engineering, Northwestern University

    Nanomaterials

    Lecture 6: Carbon Nanomaterials

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    Department of Materials Science and Engineering, Northwestern University

    7 nm

    STM Image

    AFM Image

    Carbon Nanomaterials

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    Department of Materials Science and Engineering, Northwestern University

    C60 was established by mass spectrographic analysis by Kroto and Smalley in 1985 C60 is called a buckminsterfullerene or buckyball due to resemblance to geodesic

    domes designed and built by R. Buckminster Fuller

    G. Timp,Nanotechnology, Chapter 7

    Fullerenes

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    Endohedral doping of fullerenes leads to the formation of a dipole moment thatinfluences solubility and other properties.

    G. Timp,Nanotechnology, Chapter 7

    Endofullerenes

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    G. Timp,Nanotechnology, Chapter 7

    Electronic Structure of Molecular and Solid C60

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    Calculated local density of states for Si(100)

    Structure of C60

    1.0

    0.8

    0.6

    0.4

    0.2

    0.0

    dI/dV(

    A.U.)

    -2 -1 0 1 2Energy (eV)

    C60Si Dangling BondH-passivated Si

    Spectroscopic variation among surface features

    70 x 70

    3-D STM Topograph

    C60

    Dangling

    Bonds

    Si

    Ge

    LUMO peak

    Single Molecule STM Spectroscopy of C60

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    G. Timp,Nanotechnology, Chapter 7

    Rolled Up From Graphene Sheets:Carbon Nanotubes

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins and Ph. Avouris, Scientific American, 283, 62 (2000).

    Carbon Nanotube Synthesis:Carbon Arc Discharge

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins and Ph. Avouris, Scientific American, 283, 62 (2000).

    Carbon Nanotube Synthesis:Chemical Vapor Deposition

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins and Ph. Avouris, Scientific American, 283, 62 (2000).

    Carbon Nanotube Synthesis:Laser Ablation

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    Department of Materials Science and Engineering, Northwestern University

    G. Timp,Nanotechnology, Chapter 7

    Chirality of Carbon Nanotubes

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    Department of Materials Science and Engineering, Northwestern University

    G. Timp,Nanotechnology, Chapter 7

    Energy Band Diagrams of Carbon Nanotubes

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins and Ph. Avouris, Scientific American, 283, 62 (2000).

    Electrical Properties of Graphite

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins and Ph. Avouris, Scientific American, 283, 62 (2000).

    Electrical Properties of Straight Nanotubes

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins and Ph. Avouris, Scientific American, 283, 62 (2000).

    Electrical Properties of Twisted Nanotubes

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    Department of Materials Science and Engineering, Northwestern University

    G. Timp,Nanotechnology, Chapter 7

    Bandgap of Semiconducting Nanotubes

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    Department of Materials Science and Engineering, Northwestern University

    MWNT bandgap is proportional to 1/d At room temperature,

    MWNTs behave like metals since d ~ 10 nm

    Only the outermost shell carries current in an undamaged MWNT

    Electrical Properties of MWNTs

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins and Ph. Avouris, Scientific American, 283, 62 (2000).

    Other Properties of SWNTs

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins and Ph. Avouris, Scientific American, 283, 62 (2000).

    Other Properties of SWNTs

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins and Ph. Avouris, Scientific American, 283, 62 (2000).

    Nanotubes as Interconnects

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    Department of Materials Science and Engineering, Northwestern University

    Although a cross-sectional view of a MWNT shows several

    cylindrical shells, only the outermost shell carries current in

    an undamaged MWNT.

    Current Carrying Capacity of MWNTs

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    Department of Materials Science and Engineering, Northwestern University

    8

    6

    4

    2

    0

    Currentdensity(x10

    13

    A/m

    2)

    1614121086420

    Electric field (x106

    V/m)

    Maximum current density: 6.8 x 1013

    A/m2

    Maximum electric field: 1.6 x 10

    7

    V/m

    Maximum current densities of potential interconnect materials: Metals: 1010 1012 A/m2

    Superconductors:Jc ~ 1012 A/m2

    MWNTs: >51013

    A/m2

    Representative MWNT I-V Curve:

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    Department of Materials Science and Engineering, Northwestern University

    Experimental method: Monitor the current as a function of time

    while stressing the MWNT at a fixed voltage.

    Before Electrical Stress

    1 m2 AFM image

    After Failure

    1 m2 AFM image

    Electrically Stressed MWNTs

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins, et al., Phys. Rev. Lett., 86, 3128 (2001).

    Multiwalled Carbon Nanotube Failure

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    Department of Materials Science and Engineering, Northwestern University

    G. Timp,Nanotechnology, Chapter 7

    Device Applications of Nanotube Junctions

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins, et al., Science, 292, 706 (2001).

    Engineering Carbon NanotubesUsing Electrical Breakdown

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    Department of Materials Science and Engineering, Northwestern University

    P. G. Collins, et al., Science, 292, 706 (2001).

    Engineering Carbon NanotubesUsing Electrical Breakdown