Page 147 - Carbon Nanotubes
P. 147

Vibrational modes of carbon nanotubes                 137
                                  I   I   1    I   I   I    I   I   ,
                            (32.12)  IRI I                                31.0
                            (28,16)  11111  I                             30.4
                                                                               n
                            (24,9)  111  I  I                             23.3
                                  I
                                     II             I               ni    22.8   ~
                                                                                0
                                                                                Y
                                     II  I   I      II              Ill1   15.5
                                     II  I  I       U               II I   15.2  -2
                                                                               n
                                      I  I1   I   I  II            I111   1.12
                                      /Ill    I     I1             11111   1.55
                                  I   I   I    I   I   L  -  L
                                 0       400      800     1200     1600
                                             Frequency  (cm-l)
                                                    (a)

                                      I    I   I    I   I   I    I   I
                                   I I1                              I    31.0
                                   111                               I    30.4
                                                                          23.3  0s
                                                                                n
                                    IR               I               n
                                    I II             I               I    22.8
                                                                                h
                                                                                Q)
                                                                                u
                                    I  I1                            II   15.5   i
                                    I  II                           II    15.2  .z
                                                                                n
                                      I  II          II             I II   7.72
                                       I  I1         II             111   1.55

                                      I    I   I    I   I   I    I   I
                                         400      800      1200    1600
                                              Frequency  (cm-I)
                                                    (b)
                 Fig. 4.  Diameter dependence of the first order (a) IR-active and, (b) Raman-active mode frequencies for
                                              “chiral” nanotubes.


           4.1  Synthesis and purification            as discussed in section 2. It is very desirable, therefore,
             Nested carbon nanotubes, consisting of closed con-  to remove as much of these impurity carbon phases as
           centric, cylindrical tubes were first observed by Iijima   possible. Successful purification schemes that exploit
           by TEM[37]. Later TEM studies[38] showed that the   the greater oxidation resistance of carbon nanotubes
           tubule ends were capped by the inclusion of pentagons  have  been  investigated [40-421.  Thermogravimetric
           and that the tube walls were separated by -3.4  A. A  analyses  reveal weight loss rate maxima  at 420”C,
           dc carbon-arc discharge technique for large-scale syn-   585°C) and 645°C associated with oxidation (in air)
           thesis of nested nanotubes was subsequently reported   of fullerenes, amorphous carbon soot, and graphite,
           [39]. In this technique, a dc arc is struck between two  respectively, to form volatile CO and/or  COz. Nano-
           graphite electrodes under an inert helium atmosphere,   tubes and onion-like nanoparticles were found to lose
           as is done in fullerene generation. Carbon vaporized   weight rapidly at higher temperatures around 695°C.
           from the anode condenses on the cathode to form a   Evidently, the concentration of these other forms of
           hard, glassy outer core of  fused carbon and a soft,  carbon can be lowered by oxidation.  However,  the
           black inner core containing a high concentration of   abundant carbon nanoparticles, which are expected to
           nanotubes and nanoparticles. Each nanotube typically  have a Raman spectrum similar to that shown in Figs. Id
           contains between 10 and 100 concentric tubes that are  or IC are more difficult to remove in this way. Never-
           grouped in “microbundles” oriented axially within the  theless, Ebbesen et al. [43] found that, by heating core
           core[l4].                                  material to 700°C in air until more than 99% of the
             These nested nanotubes may be harvested from the   starting material had been removed by oxidation, the
           core by grinding and sonication; nevertheless, substan-  remaining  material  consisted  solely of  open-ended,
           tial fractions of  other types of carbon remain, all of   nested nanotubes. The oxidation was found to initiate
           which are capable of producing strong Raman bands   at the reactive end caps and progress toward the cen-
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