Investigation of the properties of BiFeO3/intermediate-layer structures fabricated by magnetron sputtering

2015 ◽  
Vol 57 (9) ◽  
pp. 1764-1771
Author(s):  
A. S. Kamzin ◽  
L. S. Kamzina ◽  
H. W. Chang ◽  
Y. C. Yu ◽  
S. Y. Tu
1989 ◽  
pp. 539-544
Author(s):  
S. Miura ◽  
H. Tsuge ◽  
T. Yoshitake ◽  
S. Matsubara ◽  
T. Satoh ◽  
...  

Author(s):  
Pravahan Salunke ◽  
Kyle Fischbach ◽  
Sergei Yarmolenko ◽  
Ge Li ◽  
Yeo-Heung Yun ◽  
...  

In this study we explored the use of magnetron sputtering as an alternative to e-beam deposition for preparation of the alumina intermediate layer and of the metal catalyst on an oxidized Si wafer. This approach offers large area deposition of the layered substrate including the intermediate alumina layer and the final catalyst film. The effects of the substrate design on the growth of long multi-wall carbon nanotube (MWCNT) arrays by CVD (Chemical Vapor Deposition) were also explored. The CNT synthesis was carried on in a hydrogen/ethylene/water/argon environment at 750 °C for different periods of deposition time. Atomic Force Microscopy (AFM), Scanning Electron Microscopy (SEM), X-Ray Diffraction (XRD), Thermal Gravimetric Analysis (TGA) and Transmission Electron Microscopy (TEM) were employed to characterize the substrates and the CNT arrays. The study showed that for specific processing conditions the length of highly oriented CNTs strongly depends on the thickness of Al2O3 intermediate layer and on the catalyst film. The results obtained confirm that magnetron sputtering can be successfully employed as a tool for substrate preparation to grow 7 mm long CNT arrays with high purity. The aligned nanotubes do not suffer from limitations typical for powdered (spaghetti type) nanotubes which opens up new applications.


2009 ◽  
Vol 23 (16) ◽  
pp. 3331-3348 ◽  
Author(s):  
Q. R. HOU ◽  
W. ZHAO ◽  
Y. B. CHEN ◽  
Y. J. HE

N-type polycrystalline higher manganese silicide ( MnSi 1.7) films are prepared on thermally oxidized silicon substrates by magnetron sputtering. MnSi 1.85, Si , and carbon targets are used in the experiments. By co-sputtering of the MnSi 1.85 and Si targets, n-type MnSi 1.7 films are directly obtained. By increasing the Si content to the deposited films, both the Seebeck coefficient and electrical resistivity increase to high values. A Si intermediate layer between the MnSi 1.7 film and substrate plays an important role on the electrical properties of the films. Without the interlayer, the Seebeck coefficient is not stable and the electrical resistivity is higher. For preparation of MnSi 1.7 films by solid phase reaction, a sandwich structure Si / MnSi x/ Si (x < 1.7) and thermal annealing are used. A carbon cap layer is used as a doping source. With the carbon doping, the electrical resistivity of the MnSi 1.7 film decreases, while the Seebeck coefficient increases slightly. For reactive deposition, the MnSi x (x < 1.7) film is directly deposited on the heated substrate with a Si intermediate layer. By using a Si cap layer, a MnSi 1.7 film with a Seebeck coefficient of -292 μ V/K and electrical resistivity of 23 × 10-3 Ω- cm at room temperature is obtained. The power factor reaches 1636 μW/mK2 at 483 K. With such a high power factor, the n-type MnSi 1.7 material may be superior to p-type MnSi 1.7 material for the development of thermoelectric generators. Several smaller (0.036 - 0.099 eV ) and intermediate (0.10 - 0.28 eV ) activation energies are observed from the curves of logarithm of the resistivity versus reciprocal temperature. The larger activation energies (0.35 - 1.1 eV ) are consistent with the reported energy band gaps for higher manganese silicides.


Coatings ◽  
2021 ◽  
Vol 11 (10) ◽  
pp. 1187
Author(s):  
Yufei Wang ◽  
Shuangle Zhang ◽  
Zefeng Wu ◽  
Yong Fan ◽  
Huaqiang Chen ◽  
...  

Cu30Al70 and Ag30Al70 multilayer precursor films were prepared by magnetron sputtering, respectively. Then the nanoporous Cu/Ag multilayer composite films were successfully prepared by selecting the appropriate H2SO4 solution as the dealloying solution. It was found that the nanoporous structure was stable in the dealloying solution. The morphology and structure of nanoporous films are mainly related to the phase composition of precursors. The structure of nanoporous multilayers can be simply regarded as the superposition of single-layer structures. Our work shows that nanoporous multilayers can be well-prepared by magnetron sputtering combined with dealloying.


Micromachines ◽  
2019 ◽  
Vol 10 (3) ◽  
pp. 202 ◽  
Author(s):  
Nierlly Galvão ◽  
Marciel Guerino ◽  
Tiago Campos ◽  
Korneli Grigorov ◽  
Mariana Fraga ◽  
...  

Many strategies have been developed for the synthesis of silicon carbide (SiC) thin films on silicon (Si) substrates by plasma-based deposition techniques, especially plasma enhanced chemical vapor deposition (PECVD) and magnetron sputtering, due to the importance of these materials for microelectronics and related fields. A drawback is the large lattice mismatch between SiC and Si. The insertion of an aluminum nitride (AlN) intermediate layer between them has been shown useful to overcome this problem. Herein, the high-power impulse magnetron sputtering (HiPIMS) technique was used to grow SiC thin films on AlN/Si substrates. Furthermore, SiC films were also grown on Si substrates. A comparison of the structural and chemical properties of SiC thin films grown on the two types of substrate allowed us to evaluate the influence of the AlN layer on such properties. The chemical composition and stoichiometry of the samples were investigated by Rutherford backscattering spectrometry (RBS) and Raman spectroscopy, while the crystallinity was characterized by grazing incidence X-ray diffraction (GIXRD). Our set of results evidenced the versatility of the HiPIMS technique to produce polycrystalline SiC thin films at near-room temperature by only varying the discharge power. In addition, this study opens up a feasible route for the deposition of crystalline SiC films with good structural quality using an AlN intermediate layer.


1988 ◽  
Vol 53 (20) ◽  
pp. 1967-1969 ◽  
Author(s):  
S. Miura ◽  
T. Yoshitake ◽  
S. Matsubara ◽  
Y. Miyasaka ◽  
N. Shohata ◽  
...  

Author(s):  
R. W. Ditchfield ◽  
A. G. Cullis

An energy analyzing transmission electron microscope of the Möllenstedt type was used to measure the electron energy loss spectra given by various layer structures to a spatial resolution of 100Å. The technique is an important, method of microanalysis and has been used to identify secondary phases in alloys and impurity particles incorporated into epitaxial Si films.Layers Formed by the Epitaxial Growth of Ge on Si Substrates Following studies of the epitaxial growth of Ge on (111) Si substrates by vacuum evaporation, it was important to investigate the possible mixing of these two elements in the grown layers. These layers consisted of separate growth centres which were often triangular and oriented in the same sense, as shown in Fig. 1.


Author(s):  
G.F. Bastin ◽  
H.J.M. Heijligers ◽  
J.M. Dijkstra

For the calculation of X-ray intensities emitted by elements present in multi-layer systems it is vital to have an accurate knowledge of the x-ray ionization vs. mass-depth (ϕ(ρz)) curves as a function of accelerating voltage and atomic number of films and substrate. Once this knowledge is available the way is open to the analysis of thin films in which both the thicknesses as well as the compositions can usually be determined simultaneously.Our bulk matrix correction “PROZA” with its proven excellent performance for a wide variety of applications (e.g., ultra-light element analysis, extremes in accelerating voltage) has been used as the basis for the development of the software package discussed here. The PROZA program is based on our own modifications of the surface-centred Gaussian ϕ(ρz) model, originally introduced by Packwood and Brown. For its extension towards thin film applications it is required to know how the 4 Gaussian parameters α, β, γ and ϕ(o) for each element in each of the films are affected by the film thickness and the presence of other layers and the substrate.


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