3D Auxetic Microlattices with Independently Controllable Acoustic Band Gaps and Quasi-Static Elastic Moduli

2013 ◽  
Vol 16 (4) ◽  
pp. 357-363 ◽  
Author(s):  
Sebastian Krödel ◽  
Tommaso Delpero ◽  
Andrea Bergamini ◽  
Paolo Ermanni ◽  
Dennis M. Kochmann
2015 ◽  
Vol 62 (1) ◽  
pp. 101-108 ◽  
Author(s):  
Hirofumi Ido ◽  
Hirofumi Nagao ◽  
Masaki Harada ◽  
Hideo Kato ◽  
Junko Ogiso ◽  
...  

2019 ◽  
Vol 86 (3) ◽  
pp. 30401 ◽  
Author(s):  
Hilmi Ünlü

A thermoelastic model is proposed to determine elastic strain effects on electronic properties of spherical Type I and Type II heterostructure core/shell quantum dots (QDs) as a function of dimensions of constituent semiconductors at any temperature. Proposed model takes into account the difference between lattice constants, linear expansion coefficients and anisotropy of elastic moduli (Young's modulus and Poisson's ratio) of constituent semiconductors, respectively. In analogous to lattice mismatch, we introduce so called the elastic anisotropy mismatch in heterostructures. Compressive strain acting on core (shell) side of heterointerfaces in CdSe/CdS, CdSe/ZnS, and ZnSe/ZnS QDs increases (decreases) as shell diameter is increased, which causes increase (decrease) in core bandgap as sell (core) diameter is increased in these nanostructures. Furthermore, there is a parabolic increase in conduction band offsets and core bandgaps in CdSe/CdS, CdSe/ZnS, and ZnSe/ZnS QDs and decrease in conduction band offset and core bandgap of ZnSe/CdS QD as core (shell) diameter increases for fixed shell (core) diameter. Comparison shows that using isotropic elastic moduli in determining band offsets and core band gaps gives better agreement with experiment than anisotropic elastic moduli for core bandgaps of CdSe/CdS, CdSe/ZnS, ZnSe/ZnS, and ZnSe/CdS core/shell QDs. Furthermore, we also show that the strain-modified two band effective mass approximation can be used to determine band offsets by using measured core band gaps in core/shell heterostructure QDs with Type II interface band alignment. Excellent agreement between predicted and measured core bandgaps in CdSe and ZnSe based core/shell QDs suggests that proposed model can be a good design tool for process simulation of core/shell heterostructure QDs.


2019 ◽  
Vol 60 (79) ◽  
pp. 220-230 ◽  
Author(s):  
Rebecca Schlegel ◽  
Anja Diez ◽  
Henning Löwe ◽  
Christoph Mayer ◽  
Astrid Lambrecht ◽  
...  

ABSTRACTWe compared elastic moduli in polar firn derived from diving wave refraction seismic velocity analysis, firn-core density measurements and microstructure modelling based on firn-core data. The seismic data were obtained with a small electrodynamic vibrator source near Kohnen Station, East Antarctica. The analysis of diving waves resulted in velocity–depth profiles for different wave types (P-, SH- and SV-waves). Dynamic elastic moduli of firn were derived by combining P- and S-wave velocities and densities obtained from firn-core measurements. The structural finite-element method (FEM) was used to calculate the components of the elastic tensor from firn microstructure derived from X-ray tomography of firn-core samples at depths of 10, 42, 71 and 99 m, providing static elastic moduli. Shear and bulk moduli range from 0.39 to 2.42 GPa and 0.68 to 2.42 GPa, respectively. The elastic moduli from seismic observations and the structural FEM agree within 8.5% for the deepest achieved values at a depth of 71 m, and are within the uncertainty range. Our observations demonstrate that the elastic moduli of the firn can be consistently obtained from two independent methods which are based on dynamic (seismic) and static (tomography and FEM) observations, respectively, for deeper layers in the firn below ~10 m depth.


2021 ◽  
Author(s):  
M. A. Ghebouli ◽  
B. Ghebouli ◽  
M. Fatmi ◽  
T. Chihi ◽  
S. I. Ahmed

Abstract We report computations of all properties cited in title within GGA and LDA for cubic perovskite BiGaO3. Lattice constants, bulk modulus, elastic moduli and band gaps were computed. BiGaO3 is elastically stable at room temperature and equilibrium pressure. We predicted the Debye temperature and longitudinal and transverse waves along [100], [110] ([100], [110], [111]) directions for BiGaO3. Our calculated band gap 1.92 eV predicts the semiconducting nature. The upper valence band is consisted principally of O-2p sites and a little contribution of Ga-4p and Bi-6p states. Hybridization between Ga-4p orbital with O-2p site in the upper valence band traduces that Ga–O bonds have a covalent bonding character. B/G ratio indicates that BiGaO3 is classified as ductile material. We derived mechanical parameters of BiGaO3 using Voigt, Reuss and Hill approximations. The higher absorption value provides a hint that this material is a potential candidate as a photo catalyst in the degradation of chemicals or pollutants.


1972 ◽  
Vol 39 (1) ◽  
pp. 98-102 ◽  
Author(s):  
T. R. Tauchert ◽  
A. N. Guzelsu

An ultrasonic pulse technique was used to investigate the dispersive behavior of plane harmonic waves in a boron-epoxy composite. The dependence of group velocity upon frequency is determined for longitudinal and transverse waves propagating either parallel or perpendicular to the fibers. The static elastic moduli for the composite are also obtained, and to a first approximation the material is found to be tetragonal.


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