Synthesis and structural properties of Ge nanocrystals in multilayer superlattice structure

Author(s):  
B. Zhang ◽  
S. Shrestha ◽  
P. Aliberti ◽  
M. A. Green ◽  
G. Conibeer
2012 ◽  
Vol 37 (6) ◽  
pp. 5122-5127 ◽  
Author(s):  
Kenji Iwase ◽  
Kazuhiro Mori ◽  
Akinori Hoshikawa ◽  
Toru Ishigaki

1993 ◽  
Vol 311 ◽  
Author(s):  
Bruce M. Lairson ◽  
Mark R. Visokay ◽  
Sean B. Brennan ◽  
Robert Sinclair ◽  
Bruce M. Clemens

ABSTRACTWe report structural properties of PtFe and PtCo intermetallic compounds with perpendicular magnetic anisotropy and a preferred c-axis orientation perpendicular to the film plane, formed from initially epitaxial multilayers. These materials represent particular cases of a more general class of anisotropic magnetic compounds with the CuAu(1) natural superlattice structure. They possess high magneto-optic Kerr rotations and magnetizations, suggesting them as likely candidates for magneto-optic and perpendicular magnetic recording media.


2011 ◽  
Vol 695 ◽  
pp. 598-601
Author(s):  
Gasidit Panomsuwan ◽  
Nagahiro Saito ◽  
Osamu Takai

Superlattice structure of SrTiO3and Nb-doped SrTiO3have been epitaxially grown on atomically flat surface of LaAlO3substrates by ion beam deposition method. Epitaxial superlattices were grown at 800 °C in the presence of partial oxygen pressure under optimizing growth conditions. The Nb-doped SrTiO3layers were varied from 2 to 15 unit cell thickness approximately, while SrTiO3layers are maintained at 15 unit cell thickness with 10 periods. The superlattices with various Nb-doped SrTiO3layer thicknesses were investigated using X-ray diffractometer (XRD) and atomic force microscope (AFM), in order to clearly understand structural properties and surface structure, which are significant for fabrication of the high quality superlattice structure.


2012 ◽  
Vol 14 (9) ◽  
Author(s):  
S. Parola ◽  
E. Quesnel ◽  
V. Muffato ◽  
L. Guetaz ◽  
H. Szambolics ◽  
...  

2014 ◽  
Vol 2014 ◽  
pp. 1-7 ◽  
Author(s):  
Bo Zhang ◽  
Yong Xiang ◽  
Santosh Shrestha ◽  
Martin Green ◽  
Gavin Conibeer

Ge nanocrystals (Ge-ncs) embedded in a SiO2superlattice structure were prepared by magnetron cosputtering and postdeposition annealing. The formation of spherical nanocrystals was confirmed by transmission electron microscopy and their growth process was studied by a combination of spectroscopic techniques. The crystallinity volume fraction of Ge component was found to increase with crystallite size, but its overall low values indicated a coexistence of crystalline and noncrystalline phases. A reduction of Ge-O species was observed in the superlattice during thermal annealing, accompanied by a transition from oxygen-deficient silicon oxide to silicon dioxide. A growth mechanism involving phase separation of Ge suboxides (GeOx) was then proposed to explain these findings and supplement the existing growth models for Ge-ncs in SiO2films. Further analysis of the bonding structure of Ge atoms suggested that Ge-ncs are likely to have a core-shell structure with an amorphous-like surface layer, which is composed of GeSiO ternary complex. The surface layer thickness was extracted to be a few angstroms and equivalent to several atomic layer thicknesses.


2006 ◽  
Vol 100 (11) ◽  
pp. 114317 ◽  
Author(s):  
I. D. Sharp ◽  
Q. Xu ◽  
D. O. Yi ◽  
C. W. Yuan ◽  
J. W. Beeman ◽  
...  

2010 ◽  
Vol 518 (19) ◽  
pp. 5483-5487 ◽  
Author(s):  
B. Zhang ◽  
S. Shrestha ◽  
P. Aliberti ◽  
M.A. Green ◽  
G. Conibeer

Author(s):  
S. M. L. Sastry

Ti3Al is an ordered intermetallic compound having the DO19-type superlattice structure. The compound exhibits very limited ductility in tension below 700°C because of a pronounced planarity of slip and the absence of a sufficient number of independent slip systems. Significant differences in slip behavior in the compound as a result of differences in strain rate and mode of deformation are reported here.Figure 1 is a comparison of dislocation substructures in polycrystalline Ti3Al specimens deformed in tension, creep, and fatigue. Slip activity on both the basal and prism planes is observed for each mode of deformation. The dominant slip vector in unidirectional deformation is the a-type (b) = <1120>) (Fig. la). The dislocations are straight, occur for the most part in a screw orientation, and are arranged in planar bands. In contrast, the dislocation distribution in specimens crept at 700°C (Fig. lb) is characterized by a much reduced planarity of slip, a tangled dislocation arrangement instead of planar bands, and an increased incidence of nonbasal slip vectors.


Author(s):  
Y. H. Liu

Ordered Ni3Fe crystals possess a LI2 type superlattice similar to the Cu3Au structure. The difference in slip behavior of the superlattice as compared with that of a disordered phase has been well established. Cottrell first postulated that the increase in resistance for slip in the superlattice structure is attributed to the presence of antiphase domain boundaries. Following Cottrell's domain hardening mechanism, numerous workers have proposed other refined models also involving the presence of domain boundaries. Using the anomalous X-ray diffraction technique, Davies and Stoloff have shown that the hardness of the Ni3Fe superlattice varies with the domain size. So far, no direct observation of antiphase domain boundaries in Ni3Fe has been reported. Because the atomic scattering factors of the elements in NijFe are so close, the superlattice reflections are not easily detected. Furthermore, the domain configurations in NioFe are thought to be independent of the crystallographic orientations.


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