some arrangmentsof carbon types of swnt

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15- 398 lecture 5 © 2004 Seth Copen Goldstein 1 lecture 8 15-398 © 2004 Seth Copen Goldstein 1 Carbon Nanotubes Seth Copen Goldstein [email protected] CMU 15- 398 Introduction to Nanotechnology lecture 8 15-398 © 2004 Seth Copen Goldstein 2 Basics CNTs come in two basic flavors Single walled Multi- walled CNTs are basically rolled up Graphite http://www.photon.t.u- tokyo.ac.jp/~maruyama/agallery/agallery.html lecture 8 15-398 © 2004 Seth Copen Goldstein 3 Some Arrangments of Carbon lecture 8 15-398 © 2004 Seth Copen Goldstein 4 Types of SWNT Carbon Nanotubes

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Page 1: Some Arrangmentsof Carbon Types of SWNT

15-398 lecture 5

© 2004 Seth Copen Goldstein 1

lecture 8 15-398 © 2004 Seth Copen Goldstein 1

Carbon Nanotubes

Seth Copen [email protected]

CMU

15-398 Introduction to Nanotechnology

lecture 8 15-398 © 2004 Seth Copen Goldstein 2

Basics

CNTs come in two basic flavorsSingle walledMulti-walled

CNTs are basically rolled up Graphite

http://www.photon.t.u-tokyo.ac.jp/~maruyama/agallery/agallery.html

lecture 8 15-398 © 2004 Seth Copen Goldstein 3

Some Arrangments of Carbon

lecture 8 15-398 © 2004 Seth Copen Goldstein 4

Types of SWNT

Carbon Nanotubes

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15-398 lecture 5

© 2004 Seth Copen Goldstein 2

lecture 8 15-398 © 2004 Seth Copen Goldstein 5

A Graphene Sheet

http://ipn2.epfl.ch/CHBU/NTbasics1.htmlecture 8 15-398 © 2004 Seth Copen Goldstein 6

An Armchair nanotube (10,10)

http://www.photon.t.u-tokyo.ac.jp/~maruyama/agallery/agallery.html

lecture 8 15-398 © 2004 Seth Copen Goldstein 7

A chiral nanotube (10,5)

lecture 8 15-398 © 2004 Seth Copen Goldstein 8

Geometries

Length: can be > 1 mDiameter:

down to 1nm (SWNT)Upto 50nm (MWNT)

Tubes formed from hexagonsEnds from pentagons and hexagons(1/2 a fullerene)Open and closedBranching possible

http://ipn2.epfl.ch/CHBU/NTbasics1.htm

The Wondrous World of Carbon Nanotubes

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Calculating Diameter of SWNT

SWNT structure can be 1. (n,m) Armchair2. (n,m) Zigzag3. (n,m) ChiralWhere (n,m) are found with:

R = na1 + ma2

The diameter is found with:d = (n2 + m2 + nm)1/20.0783nm

Dai, H. Dai, H. Acc. Chem. ResAcc. Chem. Res. . 20022002, , 3535, 1035, 1035--1044.1044.

lecture 8 15-398 © 2004 Seth Copen Goldstein 10

Basic Properties

ChemicalConductors and semiconductorsStiffFlexibleThermal conduction

lecture 8 15-398 © 2004 Seth Copen Goldstein 11

Manufacturing

Many methods (covered last time)Ball millingLaser ablationPlasma arcEtc.

Result is a messPurification necessary

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Purification: WhySoot has many contaminants:

Catalyst particlesCarbon clustersSmaller fullerenes: C60 / C70

Even the NTs are mixedConducting, semiconductinSNT and MWNTDiameters, lengths

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Purification: HowRemoval of catalyst:

Acidic treatment (+ sonication)Thermal oxidationMagnetic separation (Fe)

Removal of small fullerenesMicro filtrationExtraction with CS2

Removal of other carbonaceous impuritiesThermal oxidationSelective functionalisation of nanotubesAnnealing

Main issuesNot to damage or modify the CNTsEconomics

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Conductance

Conducting or semiconducting?(n-m)/3 = 0 mod 3 -> conductingOtherwise -> semiconducting

Method of conduction?Not the same as bulk metalBallistic (Fermi-liquid)

Current Densities109A/cm2! 1000x better than copper!What does this mean when diam = 2nm?

lecture 8 15-398 © 2004 Seth Copen Goldstein 15

Mechanical Properties

Young s modulos in GigaPascals!

J.-P. Salvetat et al., Adv. Mater. 11, 161 (99).lecture 8 15-398 © 2004 Seth Copen Goldstein 16

Some Applications

Electronic NanotechnologyField-Effect DisplaysCompositesSensorsEnergy StorageSupercapacitorsAFM tips

The Wondrous World of Carbon Nanotubes

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Single nanotubes

Pull-out and release of MWNT Van der WaalsforceWorld s smallest balance

Weighing a 22 fg particleScience 283, 1513(1999)Applying hf voltage got frequency for resonance

lecture 8 15-398 © 2004 Seth Copen Goldstein 18

Hydrogen Storage

Can CNTs can be used to store hydrogen?Why?

Zero emissions

Why not?Compare Energy density3 MJ/l (5000 psi H2) vs. 32 MJ/l (gasoline)

Use: Fuel container (e.g., fuel cell) to replace use of hydrocarbons (e.g., oil)DOE minimum: 6.5% of Weight

lecture 8 15-398 © 2004 Seth Copen Goldstein 19

Two Basic Methods

Gas phase (physisorption)Van der walls bonds Room TemperatureHigher %wt (between 0-14?)

Electrochemical adsorptionElectrically dissassociate H2 from OH2 adsorbs into C

lecture 8 15-398 © 2004 Seth Copen Goldstein 20

Field-effect displays

Generates large fieldsLarge aspect ratioLarge current densities

Use as electron source in Flat-panel

Schematic structure of nanotube flat panel display.(Choi et al.)Samsung display 1999

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CNTs for interconnect

High current densitiesLow resistance (6.2K ohm)Ballistic behaviorHowever,

InductanceContact resistanceassembly

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Measuring the resistance

Note quantization of conductance

Bachtold

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MWNT resistance

Frank et al., Science 280, 1744 (1998)

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off

on

On - off state controlled by nanotube contactHysteresis in both states

Off - Elastic restoring forceOn - van der Waals attractive force

Crosstalk and addressing are still problems

C. Lieber, et al., Science 2000, 289, 94.

SWCN Crosspoint Memory

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Nanotube transistor

S.J. Tans et al., Nature 393, 49 (1998).lecture 8 15-398 © 2004 Seth Copen Goldstein 26

Carbon Nanotube FETs

IBM Nanoletters

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Using CNTs in circuits

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CNT Sensors

J. Kong et al., Science 287, 622 (2000).

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Next Time

Lets pop up a levelNanocomputing

Paper will be posted on the web

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