Page 123 - Carbon Nanotubes
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Properties of  buckytubes and derivatives             113
                                                   multilayer buckytubes. Because the insertion of pent-
                                                   agons and heptagons produced positive and negative
                                                   curvature of the hexagonal network, respectively, the
                                                   complicated morphologies of single-shell buckytubes
                                                   were probably a result of the insertion of  pentagons,
                                                   heptagons,  or various combinations into the single-
                                                   shell buckytube. We believe that it is much easier to in-
                                                   corporate pentagonal and heptagonal defects in these
                                                   single-shell structures than in multilayer buckytubes.

                                                   3.2  Magnetic properties
                                                      In the first paper reporting the observation of  c60,
                                                   Kroto et al. suggested that the molecule was aromatic-
                                                   like with its inner and outer surfaces covered with a
                                                   “sea” of a-electrons[ 181. Accordingly, Cm should ex-
                                                   hibit a large diamagnetic susceptibility associated with
                                                   a a-electron ring current. This suggestion appeared to
                                                   be supported by NMR chemical shift measurements
                                                   [ 19,231. Theoretical calculations of the magnetic sus-
                                                   ceptibility of  c60  performed by various groups were
                                                   not consistent; some authors predicted a vanishingly
                                                   small diamagnetism[24-261 and others predicted strong
                                                   diamagnetism (as in an aromatic system)[27,28]. Sus-
                                                   ceptibility measurements on C60 and C,o showed that
                                                   the value  for C,,,  was about twice that  of  c60, but
                                                   that both were very sma11[25,29]. Another theoretical
                                                   calculation by Ajiki & Ando[30] showed that the cal-
                                                   culated magnetic susceptibility for the magnetic field
                                                   perpendicular to the carbon nanotube axis was about
                                                   three  orders  of  magnitude  larger  than  the  parallel
                                                   value.  It is, then, of  interest  to extend the measure-
                                                   ments to buckytubes.
                                                      With  the availability  of  bulk  samples of  carbon
                                                   nanotubes (bundles of buckytubes), a systematic study
                                                   of  the magnetic properties became possible. A cylin-
                                                   drical bulk deposit, with a diameter of  10 mm, con-
                                                   sisting of  an inner core and an outer cladding, was
        Fig. 2.  Two HREM images of frozen growth of buckytubes   formed on the graphite cathode during the arc process.
                        seen end-on.
                                                   The outer cladding, a gray shell, was composed mainly
                                                   of amorphous carbon and buckydoughnuts[3 11. The
                                                   inner core, with a diameter of 8 mm, consisted of an
        single-crystal  growth  through  a  screw  dislocation  array of  rather evenly spaced,  parallel,  and closely
        mechanism[2].                              packed bundles approximately 50 micrometers in di-
           3.1.3  The structure  of  single-shell  bucky-  ameter. HREM revealed that the buckybundles in our
        tubes.  Single-shell buckytubes were first synthesized   best  sample were comprised of  buckytubes running
        by  Iijima and Ichihashi[20] and Bethune et al. [21].   parallel to one another[32]. A buckytube in each bun-
        Unlike their reports, where the single-shell buckytubes   dle could be pictured  as a  rolled-up graphitic  sheet
        were found on the chamber  wall, we  found a large   with  a  diameter  ranging  from 8 A to 300 A  and a
        number of monolayer buckytubes in a deposited rod   length of a few microns. The tube was capped by sur-
        which built up on the cathode of the dc arc[22]. The   faces  involving  6  pentagons  (per  layer)  on  each
        synthesis of  the single-shell buckytubes used in this   end[l,2]. The purity of the bulk sample was examined
        study was similar to that described in the experimen-   by  energy  dispersive  X-ray  analysis.  No  elements
        tal  section.  However,  instead of  using a monolithic   heavier than carbon were observed.  The C60 powder
        graphite anode, we utilized a composite anode consist-  was extracted from the soot formed in the same cham-
        ing of copper rods inserted inside a graphite anode in  ber employed for production of the buckytubes.  The
         a variety of ways. The single-shell buckytubes assumed  purity of  the c60  powder used in this study was bet-
         a large variety of  shapes (shown in Fig. 4),  such as  ter than 99% as examined by high-performance liq-
         buckytents,  buckydomes,  and giant  fullerenes,  and   uid chromatography.
         much shorter tubes than in previous reports.  Protru-   The measured mass susceptibility values for bucky-
         sions, indentations, and bending were quite common,   bundle  (both x:  and xi), C6,,, the gray-shell mate-
         unlike the faceted or smooth-faceted morphologies of  rial,  the  polycrystalline  graphite  anode,  and  the
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