35 research outputs found
Catalyst composition and impurity-dependent kinetics of nanowire heteroepitaxy.
The mechanisms and kinetics of axial Ge-Si nanowire heteroepitaxial growth based on the tailoring of the Au catalyst composition via Ga alloying are studied by environmental transmission electron microscopy combined with systematic ex situ CVD calibrations. The morphology of the Ge-Si heterojunction, in particular, the extent of a local, asymmetric increase in nanowire diameter, is found to depend on the Ga composition of the catalyst, on the TMGa precursor exposure temperature, and on the presence of dopants. To rationalize the findings, a general nucleation-based model for nanowire heteroepitaxy is established which is anticipated to be relevant to a wide range of material systems and device-enabling heterostructures.S.H. acknowledges funding from ERC grant InsituNANO (No. 279342). A.D.G. acknowledges funding from the Marshall Aid Commemoration Commission and the National Science Foundation. C.D. acknowledges funding from the Royal Society. A portion of the research was also performed using EMSL, a national scientific user facility sponsored by the Department of Energy’s (DOE) Office of Biological and Environmental Research and located at Pacific Northwest National Laboratory (PNNL). PNNL is operated by Battelle for the U.S. DOE under Contract DE-AC05-76RL01830. We gratefully acknowledge the use of facilities within the LeRoy Eyring Center for Solid State Science at Arizona State University. This work was performed in part at CINT, a U.S. DOE, Office of Science User Facility. The research was funded in part by the Laboratory Directed Research and Development Program at LANL, an affirmative action equal opportunity employer operated by Los Alamos National Security, LLC, for the National Nuclear Security Administration of the U.S. DOE under Contract DE-AC52-06NA25396.This document is the Accepted Manuscript version of a Published Work that appeared in final form in ACS Nano, copyright © American Chemical Society after peer review and technical editing by the publisher. To access the final edited and published work see http://pubs.acs.org/doi/abs/10.1021/nn402208p. Gamalski AD, Perea DE, Yoo J, Li N, Olszta MJ, Colby R, Schreiber DK, Ducati C, Picraux ST, Hofmann S, ACS Nano 2013, 7 (9), 7689–7697, doi:10.1021/nn402208
Enhanced Lithium Ion Battery Cycling of Silicon Nanowire Anodes by Template Growth to Eliminate Silicon Underlayer Islands
It
is well-known that one-dimensional nanostructures reduce pulverization
of silicon (Si)-based anode materials during Li ion cycling because
they allow lateral relaxation. However, even with improved designs,
Si nanowire-based structures still exhibit limited cycling stability
for extended numbers of cycles, with the specific capacity retention
with cycling not showing significant improvements over commercial
carbon-based anode materials. We have found that one important reason
for the lack of long cycling stability can be the presence of milli-
and microscale Si islands which typically form under nanowire arrays
during their growth. Stress buildup in these Si island underlayers
with cycling results in cracking, and the loss of specific capacity
for Si nanowire anodes, due to progressive loss of contact with current
collectors. We show that the formation of these parasitic Si islands
for Si nanowires grown directly on metal current collectors can be
avoided by growth through anodized aluminum oxide templates containing
a high density of sub-100 nm nanopores. Using this template approach
we demonstrate significantly enhanced cycling stability for Si nanowire-based
lithium-ion battery anodes, with retentions of more than ∼1000
mA·h/g discharge capacity over 1100 cycles
Silicon Nanowire Degradation and Stabilization during Lithium Cycling by SEI Layer Formation
Silicon
anodes are of great interest for advanced lithium-ion battery
applications due to their order of magnitude higher energy capacity
than graphite. Below a critical diameter, silicon nanowires enable the ∼300%
volume expansion during lithiation without pulverization. However,
their high surface-to-volume ratio is believed to contribute to fading
of their capacity retention during cycling due to solid-electrolyte-interphase
(SEI) growth on surfaces. To better understand this issue, previous
studies have examined the composition and morphology of the SEI layers.
Here we report direct measurements of the reduction in silicon nanowire
diameter with number of cycles due to SEI formation. The results reveal
significantly greater Si loss near the nanowire base. From the change
in silicon volume we can accurately predict the measured specific
capacity reduction for silicon nanowire half cells. The enhanced Si
loss near the nanowire/metal current collector interface suggests
new strategies for stabilizing nanowires for long cycle life performance
Ultrashort Channel Silicon Nanowire Transistors with Nickel Silicide Source/Drain Contacts
We demonstrate the shortest transistor channel length
(17 nm) fabricated
on a vapor–liquid–solid (VLS) grown silicon nanowire
(NW) by a controlled reaction with Ni leads on an in situ transmission
electron microscope (TEM) heating stage at a moderate temperature
of 400 °C. NiSi<sub>2</sub> is the leading phase, and the silicide–silicon
interface is an atomically sharp type-A interface. At such channel
lengths, high maximum on-currents of 890 (μA/μm) and a
maximum transconductance of 430 (μS/μm) were obtained,
which pushes forward the performance of bottom-up Si NW Schottky barrier
field-effect transistors (SB-FETs). Through accurate control over
the silicidation reaction, we provide a systematic study of channel
length dependent carrier transport in a large number of SB-FETs with
channel lengths in the range of 17 nm to 3.6 μm. Our device
results corroborate with our transport simulations and reveal a characteristic
type of short channel effects in SB-FETs, both in on- and off-state,
which is different from that in conventional MOSFETs, and that limits
transport parameter extraction from SB-FETs using conventional field-effect
transconductance measurements
Size-Dependent Silicon Epitaxy at Mesoscale Dimensions
New discoveries on collective processes
in materials fabrication
and performance are emerging in the mesoscopic size regime between
the nanoscale, where atomistic effects dominate, and the macroscale,
where bulk-like behavior rules. For semiconductor electronics and
photonics, dimensional control of the architecture in this regime
is the limiting factor for device performance. Epitaxial crystal growth
is the major tool enabling simultaneous control of the dimensions
and properties of such architectures. Although size-dependent effects
have been studied for many small-scale systems, they have not been
reported for the epitaxial growth of Si crystalline surfaces. Here,
we show a strong dependence of epitaxial growth rates on size for
nano to microscale radial wires and planar stripes. A model for this
unexpected size-dependent vapor phase epitaxy behavior at small dimensions
suggests that these effects are universal and result from an enhanced
surface desorption of the silane (SiH<sub>4</sub>) growth precursor
near facet edges. Introducing phosphorus or boron dopants during the
silicon epitaxy further decreases the growth rates and, for phosphorus,
gives rise to a critical layer thickness for single crystalline epitaxial
growth. This previously unknown mesoscopic size-dependent growth effect
at mesoscopic dimensions points to a new mechanism in vapor phase
growth and promises greater control of advanced device geometries
Gold Catalyzed Nickel Disilicide Formation: A New Solid–Liquid–Solid Phase Growth Mechanism
The
vapor–liquid–solid (VLS) mechanism is the predominate
growth mechanism for semiconductor nanowires (NWs). We report here
a new solid–liquid–solid (SLS) growth mechanism of a
silicide phase in Si NWs using in situ transmission electron microcopy
(TEM). The new SLS mechanism is analogous to the VLS one in relying
on a liquid-mediating growth seed, but it is fundamentally different
in terms of nucleation and mass transport. In SLS growth of Ni disilicide,
the Ni atoms are supplied from remote Ni particles by interstitial
diffusion through a Si NW to the pre-existing Au–Si liquid
alloy drop at the tip of the NW. Upon supersaturation of both Ni and
Si in Au, an octahedral nucleus of Ni disilicide (NiSi<sub>2</sub>) forms at the center of the Au liquid alloy, which thereafter sweeps
through the Si NW and transforms Si into NiSi<sub>2</sub>. The dissolution
of Si by the Au alloy liquid mediating layer proceeds with contact
angle oscillation at the triple point where Si, oxide of Si, and the
Au alloy meet, whereas NiSi<sub>2</sub> is grown from the liquid mediating
layer in an atomic stepwise manner. By using in situ quenching experiments,
we are able to measure the solubility of Ni and Si in the Au–Ni–Si
ternary alloy. The Au-catalyzed mechanism can lower the formation
temperature of NiSi<sub>2</sub> by 100 °C compared with an all
solid state reaction