scholarly journals Simulation of Electronic Structure of Aluminum Phosphide Nanocrystals Using Ab Initio Large Unit Cell Method

2012 ◽  
Vol 2012 ◽  
pp. 1-6 ◽  
Author(s):  
Hamad R. Jappor ◽  
Zeyad Adnan Saleh ◽  
Mudar A. Abdulsattar
Keyword(s):  
Electronic Structure ◽  
Ab Initio ◽  
Unit Cell ◽  
Aluminum Phosphide ◽  
Large Unit ◽  
Cell Method ◽  
Large Unit Cell

scholarly journals ab initio Structural, Electronic and Vibrational Properties of GaSb Nanocrystals Using Diamondoids and Large Unit Cell Method

2015 ◽  
Vol 27 (6) ◽  
pp. 2200-2204
Author(s):  
Mudar Ahmed Abdulsattar ◽  
Majed M. Mohamad
Keyword(s):  
Ab Initio ◽  
Unit Cell ◽  
Vibrational Properties ◽  
Large Unit ◽  
Cell Method ◽  
Large Unit Cell

scholarly journals Electronic Structure of Hydrogenated and Surface-Modified GaAs Nanocrystals: Ab Initio Calculations

2012 ◽  
Vol 2012 ◽  
pp. 1-5 ◽  
Author(s):  
Hamsa Naji Nasir ◽  
Mudar A. Abdulsattar ◽  
Hayder M. Abduljalil
Keyword(s):  
Electronic Structure ◽  
Ab Initio ◽  
Valence Band ◽  
Density Functional ◽  
Energy Gap ◽  
Unit Cell ◽  
Large Unit ◽  
Geometrical Optimization ◽  
Large Unit Cell ◽  
Core Part

Two methods are used to simulate electronic structure of gallium arsenide nanocrystals. The cluster full geometrical optimization procedure which is suitable for small nanocrystals and large unit cell that simulates specific parts of larger nanocrystals preferably core part as in the present work. Because of symmetry consideration, large unit cells can reach sizes that are beyond the capabilities of first method. The two methods use ab initio Hartree-Fock and density functional theory, respectively. The results show that both energy gap and lattice constant decrease in their value as the nanocrystals grow in size. The inclusion of surface part in the first method makes valence band width wider than in large unit cell method that simulates the core part only. This is attributed to the broken symmetry and surface passivating atoms that split surface degenerate states and adds new levels inside and around the valence band. Bond length and tetrahedral angle result from full geometrical optimization indicate good convergence to the ideal zincblende structure at the centre of hydrogenated nanocrystal. This convergence supports large unit cell methodology. Existence of oxygen atoms at nanocrystal surface melts down density of states and reduces energy gap.

SiGe nanocrystals core and surface electronic structure from ab initio large unit cell calculations

2011 ◽  
Vol 6 (6) ◽  
pp. 386 ◽  
Author(s):  
H.M. Abduljalil ◽  
M.A. Abdulsattar ◽  
S.R. Al-Mansoury
Keyword(s):  
Electronic Structure ◽  
Ab Initio ◽  
Unit Cell ◽  
Large Unit ◽  
Surface Electronic Structure ◽  
Large Unit Cell

Ab initio large unit cell calculations of the electronic structure of diamond nanocrystals

2011 ◽  
Vol 13 (5) ◽  
pp. 843-849 ◽  
Author(s):  
Mudar A. Abdulsattar
Keyword(s):  
Electronic Structure ◽  
Ab Initio ◽  
Unit Cell ◽  
Large Unit ◽  
Large Unit Cell

Corrections and parametrization of semiempirical large unit cell method for covalent semiconductors

2007 ◽  
Vol 75 (24) ◽  
Author(s):  
Mudar A. Abdulsattar ◽  
Khalil H. Al-Bayati
Keyword(s):  
Unit Cell ◽  
Large Unit ◽  
Cell Method ◽  
Large Unit Cell

scholarly journals Neutron diffractometer covering protein crystals with large unit cell at J-PARC

2014 ◽  
Vol 70 (a1) ◽  
pp. C1746-C1746
Author(s):  
Kazuo Kurihara ◽  
Katsuaki Tomoyori ◽  
Taro Tamada ◽  
Ryota Kuroki
Keyword(s):  
Cell Volume ◽  
Unit Cell Volume ◽  
Structural Information ◽  
Unit Cell ◽  
Proton Accelerator ◽  
Neutron Guide ◽  
Time Dimension ◽  
Hydrogen Atoms ◽  
Large Unit ◽  
Large Unit Cell

The structural information of hydrogen atoms and hydration waters obtained by neutron protein crystallography is expected to contribute to elucidation of protein function and its improvement. However, many proteins, especially membrane proteins and protein complexes, have larger molecular weight and then unit cells of their crystals have larger volume, which is out of range of measurable unit cell volume for conventional diffractometers. Therefore, our group had designed the diffractometer which can cover such crystals with large unit cell volume (target lattice length: 250 Å). This diffractometer is dedicated for protein single crystals and has been proposed to be installed at J-PARC (Japan Proton Accelerator Research Complex). Larger unit cell volume causes a problem to separate spots closer to each other in spatial as well as time dimension in diffraction images. Therefore, our proposed diffractometer adopts longer camera distance (L2 = 800mm) and selects decoupled hydrogen moderator as neutron source which has shorter pulse width. Under the conditions that L1 is 33.5m, beam divergence 0.40and crystal edge size 2mm, this diffractometer is estimated to be able to resolves spots diffracted from crystals with a lattice length of 220 Å in each axis at d-space of 2.0 Å. In order to cover large neutron detecting area due to long camera distance, novel large-area detector (larger than 300mm × 300mm) with a spatial resolution of better than 2.5mm is under development. More than 40 these detectors plan to be installed, providing the total solid angle coverage of larger than 33%. For neutron guide, ellipsoidal supermirror is considered to be adopted to increase neutron flux at the sample position. The final gain factor of this diffractometer is estimated to be about 20 or larger as compared with BIX-3/4 diffractometers operated in the research reactor JRR-3 at JAEA (Japan Atomic Energy Agency) [1,2].

Use of the Large Unit Cell Approach for Generating Special Points of the Brillouin Zone

1980 ◽  
Vol 99 (2) ◽  
pp. 463-470 ◽  
Author(s):  
R. A. Evarestov ◽  
V. P. Smirnov
Keyword(s):  
Brillouin Zone ◽  
Unit Cell ◽  
Large Unit ◽  
Large Unit Cell ◽  
Special Points
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