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An Introduction to Carbon Nanotubes

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Title: An Introduction to Carbon Nanotubes


1
An Introduction to Carbon Nanotubes
  • John Sinclair

2
Outline
  • History
  • Geometry
  • Rollup Vector
  • Metallicity
  • Electronic Properties
  • Field Effect Transistors
  • Quantum Wires
  • Physical Properties
  • Ropes
  • Separation

3
Introduction
  • High Aspect Ratio Carbon nanomaterial
  • Family inclues Bucky Balls and Graphene
  • Single Wall Carbon Nanotubes (SWCNT)
  • Multiwall Carbon Nanotubes (MWCNT)

4
History
  • 1952 L. V. Radushkevich and V. M. Lukyanovich
  • 50 nm MWCNT Published in Soviet Journal of
    Physical Chemistry
  • Cold War hurt impact of discovery
  • Some work done before 1991 but not a hot topic
  • 1991-1992 The Watershed
  • Iijima discovers MWCNT in arc burned rods
    Mintmire, Dunlap, and Whites predict amazing
    electronic and physical properties
  • 1993 Bethune and Iijima independently discover
    SWCNT
  • Add Transition metal to Arc Discharge method
    (same method as Bucky Balls)

5
Geometry
  • Rollup Vector
  • (n,m)
  • n-m3d
  • Chiral Angle
  • tan(?) v3m/(2v(n2m2nm))
  • Arm Chair (n,n), ?30 ?
  • Zig-zag (n,0), ?0 ?
  • Chiral, 0?lt ?lt30 ?

6
Field Effect Transistors
  • FETs work because of applied voltage on gate
    changes the amount of majority carriers
    decreasing Source-Drain Current
  • SWCNT and MWCNT used
  • Differences will be discussed
  • Gold Electrodes
  • Holes main carriers
  • Positive applied voltage should reduce current

7
SWCNT Transport Properties
  • Current shape consistent with FET
  • Bias VSD 10 mA
  • G(S) conductance varies by 5 orders of magnitude
  • Mobility and Hole concentration determined to be
    large
  • QCVG,T (VG,T voltage to deplete CNT of holes)
  • C calculated from physical parameters of CNT
  • pQ/eL

8
MWCNT Transport Properties
  • MWCNT performance is poor without defects
  • See arrow for twists in collapsed MWCNT
  • MWCNT has characteristic shape of FET
  • Hole density similar to SWCNT but Mobility
    determined to be higher
  • Determined same as above

9
FET Conclusions
  • Higher carrier density than graphite
  • Mobility similar to heavily p-doped silicon
  • Conductance can be modulated by 5 orders of
    magnitude in SWCNT
  • MWCNT FET only possible after structural
    deformation

10
Quantum Wires
  • SWCNT Armchair tubes
  • SWCNT deposited over two electrodes
  • Electrode resistance determined with four point
    probe and found to be 1 MO

11
Coulomb Charging
  • Contact Resistance Lower than Rquantumh/e226 kO
  • C very low s.t. ECe2/2C very large
  • If EC ltltkT, Current only flows when VbiasgtEC
  • Various gate V taken into account
  • Step-like conductance

12
Quantum Wire
  • Strongly Temperature dependent conduction curve
  • Occurs when a discrete electron level tunnels
    resonantly though Ef of electrode
  • If electron levels of SWCNT where continuous peak
    would be constant
  • E levels separated by ?E
  • The resonant tunneling implies that the electrons
    are being transported phase coherently in a
    single molecular orbital for at least the
    distance of the electrodes (140 nm)

13
Physical Properties of Ropes
  • SWCNT rope laid on ultra-filtration membrane
  • AFM tip applies force to measure Shear Modulus G
    and Reduced Elastic Modulus Er
  • Er Elastic Modulus when Searing is negligible
  • Displacement of tube/Force was measured and Er
    and G where calculated

14
Summary of Results
  • Typical Values
  • Gdia 478 GPa
  • Ggla 26.2 GPa
  • Er-dia 1220 GPa
  • Er-gla 65-90 GPa

15
Conclusion On Physical Properties
  • Shear properties of SWCNT lacking (Even compared
    to MWCNT ropes)
  • Elastic properties very promising

16
Synthesis and Seperation
  • One major reason CNT devices have been so hard to
    scale up to industry uses is due to the inability
    to efficiently separate different species of CNT
  • Different types are produced randomly with 1/3
    conducting 2/3 semiconducting
  • It has now been reported that with the use of
    structure-discriminating surfactants one can
    isolate a batch of CNT such that gt97 CNT within
    0.02 nm diameter

17
Overview of Technique
  • Surfactants change buoyancy properties of CNT
  • Ultra-centrifugation techniques (which are
    scale-able) are used to separate different CNT
  • Effective separation is seen
  • Separation according to metallicity
  • Separation according to diameter

18
Conclusion
  • CNT devices show promise in molecular electronics
    both as wires and FET
  • Physical properties are very promising being both
    strong and light
  • Separation techniques continue to be developed to
    allow companies to make CNT devices

19
Sources
  • M. S. DRESSELHAUS, G. DRESSELHAUS, and R. SAITO.
    Carbon 33, 7 (1995)
  • R. Martel, T. Schmidt, H. R. Shea, T. Hertel, and
    Ph. Avourisa. App. Phys. Lett. 73, 17 (1998)
  • Sander J. Tans, Michel H. Devoret et al. Nature
    386, 474-477 (1997)
  • Jean-Paul Salvetat et al. Phys. Rev. Lett. 82, 5
    (1999)
  • MICHAEL S. ARNOLD et al. Nature Nanotechnology 1,
    60-65 (2006)
  • www.noritake-elec.com/.../nano/structu.gif
  • http//en.wikipedia.org/wiki/Carbon_nanotube
  • academic.pgcc.edu/ssinex/nanotubes/graphene.gif
  • nano.gtri.gatech.edu/Images/MISC/figure4.gif
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