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3. Results and discussion
nanotubes, and the morphology depends strongly
on the catalysts used [9±11]. BN nanotubes are
also produced by the annealing of ball-milled B or
BN powders in nitrogen, therein Fe and Fe aust-
enite phases were observed as possible catalysts
due to the contaminant from stainless-steel con-
tainer [12,13]. Moreover, BN nanotubes and B±N±
C nanotubes were also obtained by Rao et al.
using the pyrolysis of precursor molecules over Co
catalysts [14]. These experimental results suggest
that catalysts play an important role in synthesiz-
ing BN nanotubes.
Since these techniques mentioned above are not
ideally suited for the synthesis of BN nanotubes
for applications, greater attention needs to be paid
to devise new methods. In the present Letter, we
demonstrate a simple and eective method for
growing BN nanotubes, i.e., self-selected catalytic
growth. We believe that it is useful in under-
standing the role of catalyst in the growth of BN
nanotubes.
After reaction at temperature from 1200°C to
1500°C and with 15:1 weight ratio of B=Fe2O3, a
colorless wool-like product was found on the inner
walls of the tube and boat. The amount of the
product increased with the reaction temperature.
XRD results show that the wool-like product is a
mixture of hexagonal BN +h-BN) with two-layer
repeat units and rhombohedral BN +r-BN) with
three-layer repeat units. a-Fe diraction peaks are
also observed in the XRD patterns. As the wool-
like product was collected far away from the raw
starting material, we believe that the formation of
the BN-phase must be due to a vapor-phase re-
action. In fact, when we excluded the existence of
oxygen by using iron instead of Fe2O3, the wool-
like product was not obtained. As boron has a low
vapor pressure, little boron vapor can be found
under these conditions. The vapor is likely to
contain boron oxide +B2O2 or B2O3) generated
from the reaction of boron with Fe2O3. Further-
more, TEM observations show that the wool-like
product is mainly composed of wool-like micro-
aggregates and growing in all directions like thorns
of a sea urchin. A typical HREM graph is shown
in Fig. 1a. Selected-area electron diraction and
EELSshow that the BN aggregate is amorphous.
The amorphous-phase appears in incomplete hol-
low tube form. A little of Fe +about 5% weight
ratio) can also be detected in the aggregate from
EDSmeasurements. Unfortunately, actual mor-
phologies could not be observed since it is dicult
to disperse the aggregate in an ultrasonic bath.
It is easy to observe BN nanotubes inside the
wool-like product when the reaction temperature
is lower than 1350°C, as shown in Fig. 1b. The BN
nanotubes have diameters from 7 to 20 nm, and
usually have discontinuous and variable structure,
not typically straight and cylindrical. We did not
observe metal particles at the end of BN nanotu-
bes, which is a characteristic of vapor±liquid±solid
growth mechanism [15,16]. Previous reports indi-
cate that metastable disordered amorphous
BN-phase can be converted to tubular form at
high temperature [17]. We speculate that the
observed amorphous BN aggregate be responsible
for the growth of BN nanotubes.
2. Experimental
Fe2O3 and amorphous boron powder of a pu-
rity of 95% or better were mixed in an appropriate
ratio and homogenized in an agate pestle and
mortar. An alumina boat containing the powder
mixture was placed in the central hot zone inside
an alumina tube and heated in an argon gas ¯ow.
When the reaction temperature +from 1200°C to
1500°C in our experiments) was achieved, ¯owing
ammonia gas +50 standard cubic centimeters per
minute) was introduced and reacted for 1 h.
The products were identi®ed by means of X-ray
diraction +XRD) analysis using CuKa radiation
at room temperature. Powder samples were dis-
persed in acetone using an ultrasonic bath, and a
drop of the suspension was deposited onto carbon
®lm coated grids for characterization by trans-
mission electron microscopy +TEM, Philips-
CM200), with micro-analysis via energy dispersive
spectrometry +EDS). High-resolution transmission
electron microscopy +HREM) study was carried
out in a JEM-2010 microscope operated under 200
kV, and with electron energy-loss spectrum system
+EELS).