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Implementing a NAND gate from SWCNTs

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A CNT about one nanometer in diameter bridges source and drain ... An anion-exchanged column could be used to separate bound tube and free tube. Metallic tubes ... – PowerPoint PPT presentation

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Title: Implementing a NAND gate from SWCNTs


1
Implementing a NAND gate from SWCNTs
  • Ben Gojman, Happy Hsin, Joe Liang, Natalia
    Nezhdanova, Jasmin Saini

2
Motivation
  • SWCNT Transistor
  • SWCNT Inverter

3
SWCNT Field-Effect Transistor
A semiconducting carbon nanotube supported on two
electrodes can replace the silicon channel in a
field-effect transistor.
A CNT about one nanometer in diameter bridges
source and drain electrodes, and a gating voltage
applied to the silicon substrate induces carriers
onto the nanotube to turn the transistor on.
Conductance G vs. gate voltage Vg of a p-type
semiconducting SWCNT FET
4
Intramolecular Inverter
  • Inverter built out of SWCNT
  • Protect p-type FET part of nanotube with PMMA and
    dope the exposed area to create the n-type FET

5
Experimental Results
  • Vin/Vout measured
  • Results indicate high gain as well as inverter
    behavior

6
Y-junction CNTs
  • Synthesis
  • Electronic Properties

7
Fabrication of Y-Junction Carbon Nanotubes
Pyrolysis Synthesis Method Proposed by B. C.
Satishkumar, et al

240 sccm
Outlet
Thiophene
10 sccm
Yield 70
First Furnace is heated at a rate 10 degree/min
until it reaches 623K.
Second Furnace is the Pyrolysis zone (1273K)
Pyrolysis is a form of incineration that
chemically decomposes organic materials by heat
in the absence of oxygen.
The output has carbon nanotubes, and these tubes
have multiple Y junction and can be examined
with Transmission Electron Microscope (TEM).
8
Template Synthesis Method Proposed by Jingming
Xu, et al
3 . Stem 90 nm branches 50 nm in diameter
1 .forming a Y-branched nanochannel alumina
template
2. electrochemically deposited some cobalt
catalyst in the bottom of the template channels
and reduced the catalystat 600 oC for 45 hours
under a carbon monoxide flow (100 cm3/min).
Some addition Pictures
9
Mechanical Properties Carbon Nanotubes
  • Small size
  • Low density
  • Stiff and strong
  • Conduct electricity
  • Conduct heat

10
Defining characteristics/properties
Two important features chirality diameter of
tube ? Determine whether metallic or
semiconducting
11
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12
CNTs as nanoelectronical devices
  • High mechanical strength (tensile strength 60GPa)
    and modulus (Youngs modulus 1TPa)
  • High electrical conductivity (106 ohm-1
    typically)
  • Exhibit ballistic transport
  • High thermal conductivity (1750-5800 W/mK)
  • covalently bonded and are electrical conductors
    dont suffer from electromigration or atomic
    diffusion and thus can carry high current
    densities (107 -109 A/cm2 ) 
  • Single wall nanotubes can be metallic or
    semi-conducting
  • Chemically inert, not attacked by strong acids or
    alkali

13
Necessary properties/attributes
  • Requirements
  • No rectification
  • High conductance
  • Low power dissipation
  • Current challenges
  • Fabrication
  • separation
  • Positioning
  • Physical models

14
Electronic Structure
  • Look at graphene (fused benzene)
  • Bonding p-band and anti-bonding p-band form from
    overlap between two Pz AOs
  • Expression 2-D energy states
  • W2D(kx,ky)
  • /-?014cos(?3kxa/2)cos(kya/2)4cos²(kya/2)½
  • Density of States
  • -high number in axial direction
  • -limited in circumferential direction by chiral
    vector Ch
  • Allowed (1-D quantum states) along tube axis
  • Chk 2pj j0,1,2,
  • ? Different allowed wave vectors (kmomentum e-)
    according to CNT

15
Molecular Simulation Methods-the physics-
  • Ab Initio methods
  • Obtain accurate solutions to Schrodinger equation
  • Not many exact solutions
  • Use various approximations
  • Tight binding model
  • Classical molecular dynamics
  • Solve Newtons 2nd law, particle dynamics
  • Continuum and multiscale models

16
Physics for Y junction CNTs
  • Transmission function obtained using Greens
    function formalism
  • Using tight-binding formalism for Hamiltonian and
    Greens function
  • From transmission function derive current
    properties using Landauer and Buttiker formalism
    for Quantum conductivity

17
Y junction results
Current through nanotube i
Nonlinear conductance matrix normalized to e2/h
reads
18
Symmetric Y-junction
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20
...and now, our Feature Presentation
21
NAND gate proposal
Au microwires
VDD
B
A
Vout
A
B
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250nm
32
Future Directions
  • DNA Self-Assembly

33
DNA-Assisted Disperion and Separation of Carbon
Nanotubes
WHY DNA-Assisted?
  • Carbon nanotubes are polydispersive and possess
    poor solubility in aqueous solution and
    non-aqueous solution.
  • It is discovered that DNA(ssDNA) binding to
    nanotubes is EFFECTIVE and FACILE.
  • DNA-coated nanotubes are stable for months at
    room temperature
  • Free DNA can be removed by using anion-exchange
    chromatography without disturbing the bound tube
    (strong binding).

polyT sequence
34
How DNA-Assisted?
  • ssDNA molecule are flexible within the
    sugar-phosphate backbone therefore, the molecule
    can find the low-energy conformations that
    maximize base-nanotube stacking interactions
    while exposing the sugar-P groups to water.
  • Some thermodynamics simulations were done to show
    that the binding of ssDNA onto tubes can compete
    effectively with nanotubes clinging to each other
    to form ropes.
  • Binding allows the backbone to be solvated by
    solvent and thus reduce the surface tension.
  • DNA is charged molecule and thus changes the
    charge of the bound tube. An anion-exchanged
    column could be used to separate bound tube and
    free tube.

Metallic tubes
Semi-conducting
35
References
  • Y-Junction Carbon nanotuebe, B. C. Satishkumar,
    P. J. Thomas, A. Govindraj, and C. N. R. Rao,
    Appl.Phys. Lett. 77, 2530 2000
  • Ballistic switching and rectification in single
    wall carbon nanotube Y junctions, Antonis N.
    Andriotis, APPLIED PHYSICS LETTERS VOLUME 79,
    NUMBER 2
  • Sticking of Carbon Nanotube Y Junction Branches,
    L. A. Chernozatonskii and I. V. Ponomareva, JETP
    letter, Vol.78, No.5, 2003, pp. 327-331
  • Growing Y-junction carbon nanotube, J. Li, C.
    Papadopoulos, and J. Xu, Nature London! 402, 253
    1999!.

36
Acknowledgements
  • Prof. Marc Bockrath
  • Prof. Erik Winfree

37
Questions?
JOE
38
Have a Great Summer!!!
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