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1064 nm laser irradiation. In order to obtain more information on the
formation mechanism of polyynes from suspension of graphite particles,
absorbances of polyynes in toluene are measured as a function of the
concentration of the graphite particles, the laser power, or the laser irra-
diation time at 355 nm laser irradiation. The relative abundance of polyynes
from graphite, coal, and C 60 particles is compared and their formation
mechanism from each carbon source by laser ablation in solutions is
discussed.
7.2 EXPERIMENTAL
Figure 7.1 shows a schematic view of laser ablation apparatus in solutions
used for the formation of polyynes. Small particles of graphite (Kishida
Chem. diameter 75 m m), coal (Indonesian TanitoHarum or AustralianWork-
worth), or C 60 (MER corporation) were suspended in a selected solvent. The
amount of particles used was 0.05-0.1 g per 10ml. Elemental analyses of
Tanito Harum and Workworth coals showed the following C:H:N:O ratios:
71.2:4.4:1.6:21.7%and 79.9:5.6:1.6:12.8%, respectively. As solvents, benzene,
toluene, hexane, cyclohexane, methanol, hexafluorobenzene, perfluoro-
octane, and perfluorodecaline (Kishida Chem Ind. Tokyo Kasei, or Azmax
spectral grade) were used for graphite, hexane was used for coals, and
hexane and methanol were employed for C 60 .
The experiments were performed using fundamental (1064 nm) and
frequency-multiplied outputs (532, 355, and 266 nm) of a Nd:YAG laser
(Spectra Physics GCR-100 or Continuum Surelight I-10). The energy of
the Nd:YAG laser was generally maintained at 40mJ/pulse (200mJ/cm 2 )in
FIGURE 7.1 Laser ablation cell of various kinds of carbon particles suspended in
solution.
 
 
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