382 research outputs found
Magnetic field strength influence on the reactive magnetron sputter deposition of Ta2O5
Reactive magnetron sputtering enables the deposition of various thin films to
be used for protective as well as optical and electronic applications. However,
progressing target erosion during sputtering results in increased magnetic
field strengths at the target surface. Consequently, the glow discharge, the
target poisoning, and hence the morphology, crystal structure and stoichiometry
of the prepared thin films are influenced. Therefore, these effects were
investigated by varying the cathode current Im between 0.50 and 1.00 A, the
magnetic field strength B between 45 and 90 mT, and the O2/(Ar+O2) flow rate
ratio between 0 and 100%. With increasing oxygen flow ratio a
sub-stoichiometric TaOx oxide forms at the metallic Ta target surface which
further transfers to a non-conductive tantalum pentoxide Ta2O5, impeding a
stable DC glow discharge. These two transition zones (from Ta to TaOx and from
TaOx to Ta2O5) shift to higher oxygen flow rates for increasing target
currents. Contrary, increasing the magnetic field strength (e.g., due to
sputter erosion) mainly shifts the TaOx to Ta2O5 transition to lower oxygen
flow rates while marginally influencing the Ta to TaOx transition. To allow for
a stable DC glow discharge (and to suppress the formation of non-conductive
Ta2O5 at the target) even at a flow rate ratio of 100% either a high target
current (Im >= 1 A) or a low magnetic field strength (B <= 60 mT) is necessary.
These conditions are required to prepare stoichiometric and fully crystalline
Ta2O5 films. Our investigations clearly demonstrate the importance of the
magnetic field strength, which changes during sputter erosion, on the target
poisoning and the resulting film quality.Comment: 10 pages, 9 figures, 1 tabl
Macroscopic Elastic Properties of Textured ZrN--AlN Polycrystalline Aggregates: From Ab initio Calculations to Grain-Scale Interactions
Despite the fast development of computational materials modelling,
theoretical description of macroscopic elastic properties of textured
polycrystalline aggregates starting from basic principles remains a challenging
task. In this communication we use a supercell-based approach to obtain the
elastic properties of random solid solution cubic ZrAlN system as a function of
the metallic sublattice composition and texture descriptors. The employed
special quasi-random structures are optimised not only with respect to short
range order parameters, but also to make the three cubic directions
, , and as similar as possible. In this way,
only a small spread of elastic constants tensor components is achieved and an
optimum trade-off between modelling of chemical disorder and computational
limits regarding the supercell size is achieved. The single crystal elastic
constants are shown to vary smoothly with composition, yielding
-0.5 an alloy constitution with an almost isotropic response.
Consequently, polycrystals with this composition are suggested to have Young's
modulus independent on the actual microstructure. This is indeed confirmed by
explicit calculations of polycrystal elastic properties, both within the
isotropic aggregate limit, as well as with fibre textures with various
orientations and sharpness. It turns out, that for low AlN mole fractions, the
spread of the possible Young's moduli data caused by the texture variation can
be larger than 100 GPa. Consequently, our discussion of Young's modulus data of
cubic ZrAlN contains also the evaluation of the texture typical for thin films.Comment: 10 pages, 6 figures, 3 table
Towards predictive modelling of near-edge structures in electron energy loss spectra of AlN based ternary alloys
Although electron energy loss near edge structure analysis provides a tool
for experimentally probing unoccupied density of states, a detailed comparison
with simulations is necessary in order to understand the origin of individual
peaks. This paper presents a density functional theory based technique for
predicting the N K-edge for ternary (quasi-binary) nitrogen alloys by adopting
a core hole approach, a methodology that has been successful for binary nitride
compounds. It is demonstrated that using the spectra of binary compounds for
optimising the core hole charge ( for cubic TiAlN
and for wurtzite AlGaN), the predicted spectra
evolutions of the ternary alloys agree well with the experiments. The spectral
features are subsequently discussed in terms of the electronic structure and
bonding of the alloys.Comment: 11 pages, 9 figures, 1 tabl
Graphite under uniaxial compression along the c axis: A parameter to relate out-of-plane strain to in-plane phonon frequency
Stacking graphene sheets forms graphite. Two in-plane vibrational modes of
graphite, E1u and E2g(2), are derived from graphene E2g mode, the shifts of
which under compression are all considered as results of in-plane bond
shortening. Values of Gruneisen parameter have been reported to quantify such
relation. However, the reason why the shift rates of these three modes with
pressure differ is unclear. In this work, we introduce a new parameter to
quantify the contribution of out-of-plane strain to the in-plane vibrational
frequencies, suggesting that the compression of \pi-electrons plays a
non-negligible part in both graphite and graphene under high pressure.Comment: 8 pages, 5 figures, 1 tabl
Why, what, and how? case study on law, risk, and decision making as necessary themes in built environment teaching
The paper considers (and defends) the necessity of including legal studies as a core part of built environment undergraduate and postgraduate curricula. The writer reflects upon his own experience as a lawyer working alongside and advising built environment professionals in complex land remediation and site safety management situations in the United Kingdom and explains how themes of liability, risk, and decision making can be integrated into a practical simulation in order to underpin more traditional lecture-based law teaching. Through reflection upon the writer's experiments with simulation-based teaching, the paper suggests some innovations that may better orientate law teaching to engage these themes and, thereby, enhance the relevance of law studies to the future needs of built environment professionals in practice.</p
Developing autonomous learning in first year university students using perspectives from positive psychology
Autonomous learning is a commonly occurring learning outcome from university study, and it is argued that students require confidence in their own abilities to achieve this. Using approaches from positive psychology, this study aimed to develop confidence in first‐year university students to facilitate autonomous learning. Psychological character strengths were assessed in 214 students on day one at university. Two weeks later their top three strengths were given to them in study skills modules as part of a psycho‐educational intervention designed to increase their self‐efficacy and self‐esteem. The impact of the intervention was assessed against a control group of 40 students who had not received the intervention. The results suggested that students were more confident after the intervention, and that levels of autonomous learning increased significantly compared to the controls. Character strengths were found to be associated with self‐efficacy, self‐esteem and autonomous learning in ways that were theoretically meaningful
Mesh Refinement for Anisotropic Diffusion in Magnetized Plasmas
Highly accurate simulation of plasma transport is needed for the successful
design and operation of magnetically confined fusion reactors. Unfortunately,
the extreme anisotropy present in magnetized plasmas results in thin boundary
layers that are expensive to resolve. This work investigates how mesh
refinement strategies might reduce that expense to allow for more efficient
simulation. It is first verified that higher order discretization only realizes
the proper rate of convergence once the mesh resolves the thin boundary layer,
motivating the focusing of refinement on the boundary layer. Three mesh
refinement strategies are investigated: one that focuses the refinement across
the layer by using rectangular elements with a ratio equal to the boundary
layer width, one that allows for exponential growth in mesh spacing away from
the layer, and one adaptive strategy utilizing the established Zienkiewicz and
Zhu error estimator. Across 4 two-dimensional test cases with high anisotropy,
the adaptive mesh refinement strategy consistently achieves the same accuracy
as uniform refinement using orders of magnitude less degrees of freedom. In the
test case where the magnetic field is aligned with the mesh, the other
refinement strategies also show substantial improvement in efficiency. This
work also includes a discussion generalizing the results to larger magnetic
anisotropy ratios and to three-dimensional problems. It is shown that isotropic
mesh refinement requires degrees of freedom on the order of either the layer
width (2D) or the square of the layer width (3D), whereas anisotropic
refinement requires a number on the order of the log of layer width for all
dimensions. It is also shown that the number of conjugate gradient iterations
scales as a power of layer width when preconditioned with algebraic multigrid,
whereas the number is independent of layer width when preconditioned with ILU
Tunable optoelectronic and ferroelectric properties in Sc-based III-nitrides
Sc-based III-nitride alloys were studied using Density Functional Theory with
special quasi-random structures and were found to retain wide band gaps which
stay direct up to x = 0.125 (ScxAl1-xN) and x = 0.375 (ScxGa1-xN). Epitaxial
strain stabilization prevents spinodal decomposition up to x = 0.3 (ScxAl1-xN
on GaN) and x = 0.24 (ScxGa1-xN on GaN), with critical thicknesses for strain
relaxation ranging from 3 nm to near-infinity. The increase in Sc content
introduces compressive in-plane stress with respect to AlN and GaN, and leads
to composition- and stress-tunable band gaps and polarization, and ultimately
introduces ferroelectric functionality in ScxGa1-xN at x = 0.625.Comment: 7 figures, submitte
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