scholarly journals Analyzing ab initio infrared spectra and electronic properties of polyethylenimine water complexes in the solid state

2010 ◽  
Vol 945 (1-3) ◽  
pp. 27-32 ◽  
Author(s):  
Guillaume Herlem ◽  
Tijani Gharbi ◽  
Nebiha Ben Sedrine
Keyword(s):  
Solid State ◽  
Ab Initio ◽  
Electronic Properties ◽  
Infrared Spectra

PSEUDOPOTENTIAL INVESTIGATION OF ELECTRONIC PROPERTIES OF C54- AND C49-TiSi2

2006 ◽  
Vol 20 (07) ◽  
pp. 343-351 ◽  
Author(s):  
TAO WANG ◽  
JI-AN CHEN ◽  
XING LING ◽  
YONG-BING DAI ◽  
QING-YUAN DAI
Keyword(s):  
Solid State ◽  
Plane Wave ◽  
Ab Initio ◽  
Electronic Properties ◽  
Solid State Reaction ◽  
Growth Stage ◽  
Pseudopotential Method ◽  
Generalized Gradient ◽  
Generalized Gradient Approximation

The letter casts some light on the structural, elastic and electronic properties of C49- and C54-TiSi 2, using an ab initio plane-wave ultrasoft pseudopotential method based on generalized gradient approximation (GGA). An intrinsic advantage in the growth stage for C49 phase might explain its kinetically favored phenomena in a solid-state reaction.

Morphologies and Related Electronic Properties of Carbon Nanotubes

1998 ◽  
Vol 13 (9) ◽  
pp. 2368-2379 ◽  
Author(s):  
J-C. Charlier
Keyword(s):  
Carbon Nanotubes ◽  
Solid State ◽  
Structural Optimization ◽  
Ab Initio ◽  
Electronic Properties ◽  
Graphene Sheet ◽  
Electronic Structures ◽  
Tight Binding ◽  
Electronic States

The electronic structures of different morphologies of carbon nanotubes are investigated within either tight-binding or ab initio frameworks. After a brief description of the electronic properties of the “perfect” rolled-up graphene sheet, nanotubes containing pentagon-heptagon pairs, tips (hemispherical caps), sp3-like lines responsible for polygonization, multishell and solid-state packings (bundles) are studied in order to point out the influence of such defects on the electronic states of the “perfect” cylinders. Most of the time, a structural optimization was performed on the atomic topology, prior to the calculation of the electronic properties. Connections with experimental facts are indicated as frequently as possible.

X-ray Structure Refinement and Vibrational Spectroscopy of Ca8Gd2 (PO4)6 O2

2013 ◽  
Vol 12 (10) ◽  
pp. 719-726
Author(s):  
R. Ayadi ◽  
Mohamed Boujelbene ◽  
T. Mhiri
Keyword(s):  
Solid State ◽  
General Formula ◽  
Vibrational Spectroscopy ◽  
Powder Diffraction ◽  
Infrared Spectra ◽  
Solid State Reaction ◽  
Structure Refinement ◽  
Unit Cell ◽  
Cell Group ◽  
X Ray

The present paper is interested in the study of compounds from the apatite family with the general formula Ca10 (PO4)6A2. It particularly brings to light the exploitation of the distinctive stereochemistries of two Ca positions in apatite. In fact, Gd-Bearing oxyapatiteCa8 Gd2 (PO4)6O2 has been synthesized by solid state reaction and characterized by X-ray powder diffraction. The site occupancies of substituents is0.3333 in Gd and 0.3333 for Ca in the Ca(1) position and 0. 5 for Gd in the Ca (2) position.  Besides, the observed frequencies in the Raman and infrared spectra were explained and discussed on the basis of unit-cell group analyses.

Electronic Properties and Solid-State Packing of Isocyanofulvenes and Their Gold(I) Chloride Complexes

2020 ◽  
Vol 59 (23) ◽  
pp. 17171-17183
Author(s):  
Sandra Schraff ◽  
Jens Trampert ◽  
Andreas Orthaber ◽  
Frank Pammer
Keyword(s):  
Solid State ◽  
Electronic Properties ◽  
Chloride Complexes

Direct Laser Cooling Schemes for the Triatomic SOH and SeOH Molecules Based on Ab Initio Electronic Properties

2020 ◽  
Author(s):  
Li Liu ◽  
Chuan-Lu Yang ◽  
Zhaopeng Sun ◽  
Meishan Wang ◽  
Xiano-Guang Ma
Keyword(s):  
Optical Properties ◽  
Ab Initio ◽  
Electronic Properties ◽  
Laser Cooling ◽  
Promising Method ◽  
Optical Scheme ◽  
Electronic And Optical Properties ◽  
Cold Molecules ◽  
Direct Laser

The direct laser cooling is a very promising method to obtain cold molecules for various applications. However, a molecule with satisfactory electronic and optical properties for the optical scheme is...

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