A Novel Approach for Real Mass Transformation
from V2O5 Particles to Nanorods
Alexey M. Glushenkov, Vladimir I. Stukachev, Mohd Faiz
Hassan, Gennady G. Kuvshinov, Hua Kun Liu, and Ying Chen
Crystal Growth & Design, 8(10) (2008) 3661-5
A solid-state, mass-quantity transformation from V2O5
powders to nanorods has been realized via a two-step approach. The nanorods
were formed through a controlled nanoscale growth from the nanocrystalline
V2O5 phase created by a ball milling treatment. The nanorods grow along
the [010] direction and are dominated by {001} surfaces. Surface energy
minimization and surface diffusion play important roles in their growth
mechanism. Real large quantity production can be achieved when the annealing
process is conducted in a fluidized bed which can treat large quantities
of the milled materials at once. The crystal orientation of nanorods provides
an improved cycling stability for lithium intercalation.
Growth and structure of prismatic boron nitride
nanorods
H.Z. Zhang, J. D. Fitz Gerald, L. T. Chadderton, J. Yu,
Y. Chen
Physical Review B 74(1)(2006) 045407
Growth takes place by rapid surface diffusion of BN molecules,
and follows heterogeneous nucleation at catalytic particles of an Fe/Si
alloy. Lattice imaging transmission electron microscopy studies reveal a
central axial row of rather small truncated pyramidal nanovoids on eachnanorod,
surrounded by three basal planar BN domains which, with successive deposition
of epitaxial layers adapt to the void geometry bycrystallographic faceting.
The bulk strain in the nanorods is taken up by the presence of what appear
to be simple nanostacking faults in theexternal, near-surface domains which,
like the nanovoids are regularly repetitive along the nanorod length. Growth
terminates with a clearcuneiform tip for each nanorod. Lateral nanorod dimensions
are essentially determined by the size of the catalytic particle, which
remains as afoundation essentially responsible for base growth. Growth,
structure, and dominating facets are shown to be consistent with a system
which seekslowest bulk and surface energies according to the well-known
thermodynamics of the capillarity of solids.
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(a) Lattice images of the nanorods (b) Corresponding electrondiffraction
pattern (c) the distribution of the apex angles (d) thecomposition of the
nanorods: B and N only.
PatternedGrowth and Cathodoluminescence
of Conical Boron Nitride Nanorods
H.Z. Zhang, M. Phillips, J. Fitz Gerald, J. Yu, Y. Chen,
Appl. Phys. Lett. 88 (2006) 093117
Cathodoluminescence (CL) spectra of the nanorods show two broad emission
bands centered at 3.75 and 1.85 eV. Panchromatic CL images reveal
clear patterned structure. ©2006 American Institute of Physics
Conical Boron NitrideNanorods Synthesized Via the Ball-Milling
and Annealing Method
H.Z. Zhang, J. Fitz Gerald, J. Yu, Y. Chen,
Journal of the American Ceramic Society 89 (2006) 675-679
Nanorods: A boron nitride (BN) nanostructure, conical BN
nanorod, has been synthesized in a large quantity on Si substrates for the
first time viathe ball-milling and annealing method. Nitridation of milled
boron carbide (B4C) powders was performed in nitrogen gas at 1300°C
on the surface of thesubstrates to form the BN nanorods. The highly crystallized
nanorods consist of conical BN basal layers stacked along the nanorod axis.
Ball milling ofthe B4C powders can significantly enhance the nitridation
of the powders and thus facilitate the formation of nanorods during the
annealing process.(2) Patterned growth: A catalyst layer of Fe(NO3)3
was patterned on a silicon substrate by using a copper grid as a mask. The
nanorods were grownvia annealing milled boron carbide powders at 1300
°C in a flow of nitrogen gas. The as-grown nanorods exhibit uniform
morphology and the catalystpattern precisely defines the position of nanorod
deposition.
1.Milling-effect:
(a) XRD pattern shows the milled B4C powder having smallcrystallite
sizes; (b) Enhanced nitridation of the milled B4C powder
2.Morphology:
(a) The BN nanorods are grown on the silicon substrate on alarge sacle. The nanorods have (b) conical tips and (c) bulbousattachment(catalyst particles)
J. Phys. D: Appl. Phys.(2006), Accepted.
The emission current of the BN nanorods can be up to $\sim$
60 $\mu$A at an applied voltage of $\sim$ 3 kV. Two distinct slopes are evident
in the Fowler-Nordheim (FN) plot. The field-emission characteristics can be
explained using a site-related tunneling-controlled mechanism. The occurrence
of two FN slopes is attributed to the switchover from tipemission to side
emission, which results from the differences in interface barrier, geometry,
as well as total emission area of the two emission interfaces.