Perforation-rotation based approach for band gap creation and enlargement in low porosity architected materials

2020 ◽  
Vol 245 ◽  
pp. 112331
Author(s):  
Xiangyu Tian ◽  
Wenjiong Chen ◽  
Renjing Gao ◽  
Shutian Liu ◽  
Jiaxing Wang
Keyword(s):  
Band Gap ◽  
2011 ◽  
Vol 20 (01) ◽  
pp. 153-160 ◽  
Author(s):  
A. DOBRINSKY ◽  
A. SADRZADEH ◽  
B. I. YAKOBSON ◽  
J. XU

Graphene nanoribbons exhibit band gap modulation when subjected to strain. While band gap creation has been theoretically investigated for uniaxial strains, other deformations such as nanoribbon twist have not been considered. Our main objective in this paper is to explore band gap opening in twisted graphene nanoribbons that have metallic properties under tight-binding approximation. While simple considerations based on the Hückel model allow to conclude that zigzag graphene nanoribbons exhibit no band gap when subjected to twist, the Hückel model overall may be inaccurate for band gap prediction in metallic nanoribbons. We utilize Density Functional Theory Tight-Binding Approximation together with a requirement that energy of twisted nanoribbons is minimized to evaluate band gap of metalic armchair nanoribbons. Besides considering twisting deformations, we also explore the possibility of creating band gap when graphene nanoribbons are subject to inhomogeneous deformation such as sinusoidal deformations.


2006 ◽  
Vol 119 (5) ◽  
pp. 3410-3411
Author(s):  
Vicent Romero Garcia ◽  
Elies Fuster Garcia ◽  
Juan V. Sanchez‐Perez ◽  
Luis M. Garcia‐Raffi ◽  
Enrique A. Sanchez‐Perez
Keyword(s):  
Band Gap ◽  

2007 ◽  
Vol 90 (24) ◽  
pp. 244104 ◽  
Author(s):  
E. Fuster-Garcia ◽  
V. Romero-García ◽  
J. V. Sánchez-Pérez ◽  
L. M. García-Raffi
Keyword(s):  
Band Gap ◽  

2006 ◽  
Vol 88 (17) ◽  
pp. 174104 ◽  
Author(s):  
V. Romero-García ◽  
E. Fuster ◽  
L. M. García-Raffi ◽  
E. A. Sánchez-Pérez ◽  
M. Sopena ◽  
...  
Keyword(s):  
Band Gap ◽  

Author(s):  
Joanna L. Batstone

Interest in II-VI semiconductors centres around optoelectronic device applications. The wide band gap II-VI semiconductors such as ZnS, ZnSe and ZnTe have been used in lasers and electroluminescent displays yielding room temperature blue luminescence. The narrow gap II-VI semiconductors such as CdTe and HgxCd1-x Te are currently used for infrared detectors, where the band gap can be varied continuously by changing the alloy composition x.Two major sources of precipitation can be identified in II-VI materials; (i) dopant introduction leading to local variations in concentration and subsequent precipitation and (ii) Te precipitation in ZnTe, CdTe and HgCdTe due to native point defects which arise from problems associated with stoichiometry control during crystal growth. Precipitation is observed in both bulk crystal growth and epitaxial growth and is frequently associated with segregation and precipitation at dislocations and grain boundaries. Precipitation has been observed using transmission electron microscopy (TEM) which is sensitive to local strain fields around inclusions.


Author(s):  
J.M. Bonar ◽  
R. Hull ◽  
R. Malik ◽  
R. Ryan ◽  
J.F. Walker

In this study we have examined a series of strained heteropeitaxial GaAs/InGaAs/GaAs and InGaAs/GaAs structures, both on (001) GaAs substrates. These heterostructures are potentially very interesting from a device standpoint because of improved band gap properties (InAs has a much smaller band gap than GaAs so there is a large band offset at the InGaAs/GaAs interface), and because of the much higher mobility of InAs. However, there is a 7.2% lattice mismatch between InAs and GaAs, so an InxGa1-xAs layer in a GaAs structure with even relatively low x will have a large amount of strain, and misfit dislocations are expected to form above some critical thickness. We attempt here to correlate the effect of misfit dislocations on the electronic properties of this material.The samples we examined consisted of 200Å InxGa1-xAs layered in a hetero-junction bipolar transistor (HBT) structure (InxGa1-xAs on top of a (001) GaAs buffer, followed by more GaAs, then a layer of AlGaAs and a GaAs cap), and a series consisting of a 200Å layer of InxGa1-xAs on a (001) GaAs substrate.


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