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  • Nano-1

    Nanoscience I: Hard nanostructures

    Kai Nordlund10.10.2010

    Faculty of Science

    Department of Physics

    Division of Materials Physics

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Contents

    Carbon nanostructuresBackgroundGraphene FullerenesNanotubes

    NanoclustersBackgroundNanoclustersNanocrystalline materials

    Thin filmsBackgroundPhysical deposition methodsChemical deposition methods

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Carbon nanostructures: background

    Carbon has 3 main kinds of chemical bonding

    sp: linearE.g. acetylene molecule C2

    H2

    sp2: 3 bonds in a plane, angles of 120o

    E.g. ethylene molecule C2

    H4Graphite bulk structure

    -

    Interaction between layers weak

    (no covalent bonding)

    Single graphene sheet

    sp3: 4 bonds symmetric in 3D E.g. methane molecule CH4Diamond bulk structure

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Graphene

    Individual graphene

    sheets were first isolated as late as in 2004

    by Andre Geim

    et al. at the University of ManchesterAndre Geim

    and Konstantin Novoselov

    got the Nobel prize for the discovery in 2010!

    Isolation technique in principle very simpleSchotch

    tape and peel offEven an ordinary pencil draw will make a number if isolated

    graphene

    sheetsBut the difficult part was to get

    large areas, detect and manipulate them in a controlled manner

    Now it can be done routinely

    A single graphene

    sheet can be

    macroscopic and visible to the naked eye!

    [A. K. Geim Science 324, 1530-1534 (2009)]

  • Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Graphene properties

    An ideal 2D conducting system

    Very durable mechanically, does not oxidize in air

    Graphene

    can be grown in various ways

    e.g. on Ni and then

    transferred on Si (C) or on SiC

    (D)

    Graphene

    paper can be

    made out of graphene

    oxide

    [A. K. Geim Science 324, 1530-1534 (2009)]

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Graphene has incredible strength

    [http://static.nobelprize.org/nobel_prizes/physics/laureates/2010/sciback_phy_10.pdf]

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Relation of carbon nanostructures

    All of the carbon sp2 structures can be conceptually thought of to derive from grapheneReal growth is different!

    [http://static.nobelprize.org/nobel_prizes/physics/laureates/2010/sciback_phy_10.pdf] Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Fullerenes

    The fullerene molecule C60

    was found in 1985 Kroto, Smalley & co.

    Round carbon molecules

    Each carbon atom has 3 bonds, and the atoms form rings with 5 or 6 atoms (pentagons and hexagons) Just like in a traditional soccer football!

    Could be imagined to be formed by strongly bending a graphene sheet to a ball Bond reforming needed to form pentagons,

    though

    Name got inspiration from the architect Buckminster Fuller who designed similar domes Fullerene, Buckyball, Buckminsterfullerene

  • Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Different types of fullerenes

    Even though C60

    is the most common, many other fullerenes do also existAt least C30

    C720

    The smallest (Natoms

    < 30) are likely not closed shells, i.e.

    are not fullerenes

    The largest are no longer round They have more energetically

    favorable hexagons in flat regions

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Production

    Fullerenes can be made in many

    different ways, but the basic idea of most methods is similar to:

    Carbon sourceHigh voltage or temperature

    makes the carbon gasify The holder has He gas

    in a low pressure (e.g. 100 Torr)

    In the gas or plasma fullerenes are formed

    -

    Also ordinary soot

    Fullerenes can be dissolved

    in e.g. toluene, the soot not

    [http://www.sussex.ac.uk/Users/kroto/workshop.html]

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Fullerene properties

    Individual fullerenes are very elastically hard: The C-C bond in graphite is one of the strongest in existenceExperimental bulk modulus (capability to resist compression) ~ 1000

    GPa

    (diamond 442 GPa)

    But the bond between fullerenes is very weak (same as the so called van der

    Waals/dispersion interaction between graphite

    shells The bulk modulus of a crystal formed from fullerenes only 14 GPaMelting/boiling point 300 oC

    Interesting new chemistryAlready in 1997 over 9000 fullerene

    compounds was known

    now nobody

    is counting any more

    It is possible to put atoms or molecules inside fullerenes Endohedral

    fullerenes

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1

    Fullerene properties: superconductivity

    Maybe the most surprising property of fullerenes is that they can be made electrically superconducting Superconductivity = no electrical resistance

    For instance the K3

    C60 crystal is superconducting below 18.4 K Rubidium-Thallium-doped fullerenes have a

    transition temperature as high as 45 K

    Compare this with:Normal metals max. about 20 KCeramic copper oxide superconductors

    about 50-100 K

    Fullerene superconductors are their own class of superconducting materialsNot understood on a fundamental level!

  • Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Carbon nanotubes

    Carbon nanotubes are hollow cylindrical tubes of carbon that have a diameter of only a few nanometers, but may have lengths of micronsRecord is 4 cm length for a single tube [Zheng

    et al, Nature Materials 2004]

    Like a graphene shell rolled to a tube, all atoms in hexagons

    The end of the tube can be open or fullerene-like

    [C. Dekker, Delft Univ.]

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Chirality of carbon nanotubes

    A nanotube can conceptually be formed by rolling up a sheet of graphene so that the bonds at the edges match perfectlyA sheet can be rolled up in any wayBut a graphene sheet has bonding directions, so all directions are not

    equivalent The types of possible

    cuts can be defined by a single vector OA

    This vector can be determined from the bonding directions in graphene, vectors a1 , a2 .

    These can be used to

    form the vector OA as

    shown to the right I.e. 4 and 2 vectors: (4,2)

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Chirality of carbon nanotubes: notation

    The chirality is given by two numbers in the form (A,B), A>B E.g. the cut shown above was (4,2) and the resulting tube becomes:

    The tube clearly has a helix-shaped twisted

    form, i.e. is chiral

    Tubes with indices of the form (A,0) and (A,A) are not chiral They are thus called achiral

    Tubes of the form (A,A) are called armchair tubes

    Tubes of the form (A,0) are called zigzag tubes

    All other types are called chiral

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Nanotube chirality, examples

    (5,5) armchair

    (9,0) zigzag

    (10,5) chiral

  • Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Armchair ??

    Whence the name armchair??

    If you look at the tube from the side, you can imagine seeing the shape of an armchair on it

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Single vs. multiwalled nanotubes

    Nanotubes may have many tubes inside each otherSingle-walled nanotubes SWNT, multi-walled nanotubes MWNT

    -

    Special cases of MWNTs: double-walled: DWNT, triple-walled: TWNT

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Production of the tubes

    The basic idea of making carbon nanotubes is the same as that of fullerenesHot gas or plasma of carbon, possibly carrier gases

    Single-walled tubes require metal nanoclusters to grow!Otherwise the end closes quickly and one only gets a fullerene

    Multi-walled tubes can grow spontaneously The different walls interact with each other and prevent closure

    Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Nanotube structures

    The nanotubes can form a bundle

    And a rope can be formed from the bundlesNote the scale!

    [Zhu et al, Science 296 (2002) 884]

  • Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Nanotube forest and -paper

    By growing nanotubes from a surface one can form a forest

    out of them

    Paper can be made from the bundles Paper

    in the generalized meaning of a fiber network

    [K. Arstila. Accelerator Laboratory]Kai Nordlund, Department of Physics, University of Helsinki

    Nano-1 Properties of a single nanotube

    A single nanotube has incredibly good properties

    Strength:Youngs modulus: 1250 GPa

    -

    Cf. Fe 211 GPa

    Tensile strength: in theory 300 GPa, measured 63 GPa-

    Cf. steels 0.5

    1.5 GPa

    Electrical conductance The tubes are either metallic or semiconducting depending on

    chirality:-

    Armchair tubes (A,A) are metals-

    If A-B is divisible by three: small band-gap semiconductor-

    Otherwise: large band gap semiconductor

    Very large current-carrying capacity:Estimated at 1000 MA/c