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Fullerenes; discovery, properties and applications

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Title: Fullerenes; discovery, properties and applications


1
Fullerenes discovery, properties and applications
  • Physics 790 presentation by
  • Mustapha Habibi
  • UNR Fall 2007

2
Outline
  • History
  • Introduction
  • What are fullerenes?
  • Bonds in the sp2 hybridization.
  • How are fullerenes made?
  • Properties
  • Photo-ionization of fullerenes
  • Ion-photon merged-beams end station at ALS
  • Photo-ionization process
  • Photo-ionization of C60
  • Photo-ionization of C84
  • Comparison between the two spectra
  • Applications of fullerenes
  • Summary

3
How did we get to know about fullerenes?
  • Nuclear physics researchers Hahn Strassman in
    Germany noticed that carbon cluster ions up to
    C15 were produced in a high frequency arc with a
    graphite electrode in the 1943.
  • A Japanese physical organic chemist E. G. Osawa
    had perceived that carbon in the single layer
    closed cages structure would be aromatic and
    therefore stable, in early 1970.
  • Galpern (Russian scientist) had completed the
    first of many Hückel calculations showing that it
    would be a closed shell molecule with a large
    HOMO-LUMO gap in 1973.
  • Fullerenes were discovered experimentally for the
    first time by a group of scientists at Rice
    University, Houston, Texas, in September of 1985.

4
Photograph of the research group that discovered
the fullerenes at Rice University in September of
1985. standing Curl, kneeling (left to right)
OBrian, Smalley, Kroto and Heath
Nobel Prize in chemistry in 1996
5
What are fullerenes?
  • Fullerenes are closed hollow cages consisting of
    carbon atoms interconnected in pentagonal and
    hexagonal rings.
  • Each carbon atom on the cage surface is bonded to
    three carbon neighbors therefore is sp2
    hybridized.
  • The most famous fullerene is C60, known also by
    buckyball ".
  • Other relatively common clusters are C70, C72,
    C74, C76, C80, C82 and C84 (plenty of others,
    higher or lower than C60, exist too but less
    abundant in the experimentally produced mixture
    fullerene soot).

6
Mass spectrum of carbon clusters
R. E. Smalley, Nobel Prize lecture, December 7,
1996
7
What are fullerenes? (continued)
8
Carbon-carbon bonds in the sp2 hybridization
configuration.
  • Hybridization The mixing of atomic orbitals,
    such as s and p orbitals, to form a new, hybrid
    orbital for use in bonding.
  • Carbon virtually never uses a pure s orbital to
    bond.
  • Carbon has three different ways to hybridize
    sp3, sp2, and sp.
  • sp3 all three p orbitals are mixed in with the s
    orbital.
  • sp2only two of the p orbitals are mixed in.
  • Sp only one p atomic orbital is mixed with an s
    orbital.
  • The designation spm is intended to be a
    shortened form of s1pm.

9
How are fullerenes made?
  • Fullerenes can be made by vaporizing carbon
    within a gas medium.
  • (they could form spontaneously in a condensing
    carbon vapor)

R. E. Smalley, Nobel Prize lecture, December 7,
1996
10
Outline
  • History
  • Introduction
  • What are fullerenes?
  • Bonds in the sp2 hybridization.
  • How are fullerenes made?
  • Properties
  • Photo-ionization of fullerenes
  • Ion-photon merged-beams end station at ALS
  • Photo-ionization process
  • Photo-ionization of C60
  • Photo-ionization of C84
  • Comparison between the two spectra
  • Applications of fullerenes
  • Summary

11
Properties of fullerenes
  • No other element has such wonderful properties as
    carbon.
  • Buckyballs are relatively cheap carbon is
    everywhere!
  • Even though each carbon atom is only bonded with
    three other carbons (they are most comfortable
    with four bonds) in a fullerene molecule,
    dangling a single carbon atom next to the
    structure is not strong enough to break the
    structure of the fullerene molecule.

12
Properties of fullerenes (continued)
  • In fullerenes, 12 pentagonal rings are necessary
    and sufficient to effect the cage closure.
  • Fullerenes contain carbon atoms arranged as a
    combination of 12 pentagonal rings and n
    hexagonal rings. The chemical formula is C202n.
  • Fullerene cages are about 7-15 Å in diameter, and
    are one carbon atom thick.

13
Properties (continued)
  • Quite stable from chemical and physical points of
    view (breaking the balls requires temperatures of
    about 1000 C).
  • Highest tensile strength of any known 2D
    structure or element.
  • Highest packing density of all known structures.
  • Impenetrable to all elements under normal
    circumstances, even to a helium atom with an
    energy of 5 eV.

14
Outline
  • History
  • Introduction
  • What are fullerenes?
  • Bonds in the sp2 hybridization.
  • How are fullerenes made?
  • Properties
  • Photo-ionization of fullerenes
  • Ion-photon merged-beams end station at ALS
  • Photo-ionization process
  • Photo-ionization of C60
  • Photo-ionization of C84
  • Comparison between the two spectra
  • Applications of fullerenes
  • Summary

15
Ion-photon merged-beams endstation at the
Advanced Light Source
Beamline 10.0.1






16
Direct (non-resonant) Photoionization
8
e-
e-
e-
Ion A
Ion A
Photon A (atom, ion or molecule)
? A free electron
17
Indirect (resonant) Photoionization
8
e-
e-
e-
Ion A
Final charge 1
Photon A
? Inner shell e- of ion A jumps to an upper
energy level ( A)
? The excited e- decays back to its initial
energy level giving its excess energy to another
e- from the same upper level
? The latter gets enough energy to get away and
be free
? e- A
18
Giant Resonances
  • A giant resonance in general describes a
    collective excitation of the nucleons or
    electrons of an atom or ion.
  • Giant resonances may be excited by
    photo-absorption or by collisions.
  • The term giant resonance in atoms has also been
    applied to describe a dominant excitation that
    accounts for a significant fraction of the total
    oscillator strength.

M. Ya Amusia and J. P. Connerade, Rep. Prog.
Phys. 63, 41-70 (2000).
19
Surface Plasmon
e-
e-
1
20
Volume Plasmon
e-
1
21
Photoionization of C60 ions
22
Photoionization of C60 (continued)
Localized Molecular Excitations

23
Two distinct modes of collective oscillations of
the 239 valence electrons of the C60 molecule
due to photo-excitation are evident.
S.W.J. Scully et al., Phys. Rev. Lett. 94, 065503
(2005).
24
Fullerene ions in initially higher charge states
photoionize less readily.
25
Photoionization of C84 molecular ion.
26
(No Transcript)
27
C60 and C84 photoionization cross sections
scale with the number of C atoms.
28
Outline
  • History
  • Introduction
  • What are fullerenes?
  • Bonds in the sp2 hybridization.
  • How are fullerenes made?
  • Properties
  • Photo-ionization of fullerenes
  • Ion-photon merged-beams end station at ALS
  • Photo-ionization process
  • Photo-ionization of C60
  • Photo-ionization of C84
  • Comparison between the two spectra
  • Applications of fullerenes
  • Summary

29
Applications of fullerenes.
  • Due to their extremely resilient and sturdy
    nature, fullerenes are being considered for use
    in combat armor.
  • Researchers have found that water-soluble
    derivates of fullerenes inhibit the HIV-1
    protease (enzyme responsible for the development
    of the virus) and are therefore useful in
    fighting the HIV virus that leads to AIDS.
  • Elements can be bonded with C60 or other
    fullerenes to create more diverse materials,
    including superconductors and insulators.

30
Summary
  • Giant dipole resonances dominate the
    photoionization of fullerene molecular ions in
    the low energy range 17- 50 eV.
  • Contributions due to localized and collective
    electron excitations of fullerenes are readily
    distinguishable in photoion-yield spectra.
  • Fullerenes have many applications and are very
    useful in military, medicine, nano-technology and
    many other fields .

31
Any Questions?
32
Fullerenes discovery, properties and applications
  • Physics 790 presentation by
  • Mustapha Habibi
  • UNR Fall 2007
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