Conjugated polymers: A systematic investigation of their electronic and geometric properties using density functional theory and semi-empirical methods

2018 ◽  
Vol 246 ◽  
pp. 128-136 ◽  
Author(s):  
Khanh B. Vu ◽  
Van V. Vu ◽  
Huong Phung Thi Thu ◽  
Ha N. Giang ◽  
Nguyen Minh Tam ◽  
...  
Author(s):  
Banjo Semire ◽  
Isaiah Ajibade Adejoro ◽  
Olusegun Ayobami Odunola

In this paper, we theoretically studied the geometries, stabilities, electronic and thermodynamic properties of bridged bithiophene S-oxide (BTO-X) derivates (with X = BH2, SiH2, S, S=O, and O) by using semi-empirical methods, ab-initio, and Density functional theory. The geometries and thermodynamic parameters calculated by PM3 were in good agreement with that of B3LYP/6-31G(d). The bandgap calculated by B3LYP/6-31G(d) ranged from 3.94eV (BTO-O)-3.16eV (BTO-BH2). The absorption λmax calculated suing B3LYP/6-31G(d) shifted to longer wavelength with X=BH2, SiH2, and S=O due to enhancement of π-conjugated system whereas, BTO-S and BTO-O shifted to shorter wavelengths as compared to dimmer thiophene S-oxide (2TO).


2014 ◽  
Vol 16 (28) ◽  
pp. 14368-14377 ◽  
Author(s):  
Qiang Cui ◽  
Marcus Elstner

Semi-empirical (SE) methods are derived from Hartree–Fock (HF) or Density Functional Theory (DFT) by neglect and approximation of electronic integrals.


2018 ◽  
Vol 33 (1) ◽  
pp. 71
Author(s):  
Ali Hashem Essa ◽  
A. F. Jalbout

The structural and electronic properties of 1-(5-Hydroxymethyl - 4 –[ 5 – (5-oxo-5-piperidin- 1 -yl-penta- 1,3 -dienyl)-benzo [1,3] dioxol- 2 -yl]- tetrahydro -furan-2 -yl)-5-methy l-1Hpyrimidine-2,4dione (AHE) molecule have been investigated theoretically by performing density functional theory (DFT), and semi empirical molecular orbital calculations. The geometry of the molecule is optimized at the level of Austin Model 1 (AM1), and the electronic properties and relative energies of the molecules have been calculated by density functional theory in the ground state. The resultant dipole moment of the AHE molecule is about 2.6 and 2.3 Debyes by AM1 and DFT methods respectively, This property of AHE makes it an active molecule with its environment, that is AHE molecule may interacts with its environment strongly in solution.


Author(s):  
Michael Fischer ◽  
Robert G. Bell

AbstractDensity-functional theory calculations including a semi-empirical dispersion correction (DFT-D) are employed to study the interaction of small guest molecules (CH


2019 ◽  
Author(s):  
Alexander Tygesen ◽  
Jinhyun Chang ◽  
Tejs Vegge ◽  
Juan Maria García Lastra

Computational study of anionic redox processes in Li2MnO3, and newly developed methods for identifying and studying the evolution of anionic redox using density functional theory (DFT). A method for identifying localized anionic redox species is applied to a set of structures relaxed using the VASP software. A preconditioning scheme is presented to promote the formation of peroxo-like oxygen species, and study the formation and evolution of anionic redox.


2013 ◽  
Vol 10 (3) ◽  
pp. 1041-1049
Author(s):  
Baghdad Science Journal

Density Functional Theory (DFT) with B3LYP hybrid exchange-correlation functional and 3-21G basis set and semi-empirical methods (PM3) were used to calculate the energies (total energy, binding energy (Eb), molecular orbital energy (EHOMO-ELUMO), heat of formation (?Hf)) and vibrational spectra for some Tellurium (IV) compounds containing cycloctadienyl group which can use as ligands with some transition metals or essential metals of periodic table at optimized geometrical structures.


2016 ◽  
Vol 18 (20) ◽  
pp. 13830-13843 ◽  
Author(s):  
Seema Gautam ◽  
Abir De Sarkar

Vinyl isocyanide formation: adsorption of C2H2 and HCN in succession on the Au9 cluster; towards polymerization: clustering of C2H2 on Au9.


Molecules ◽  
2018 ◽  
Vol 23 (10) ◽  
pp. 2466 ◽  
Author(s):  
Junming Ho ◽  
Yihan Shao ◽  
Jin Kato

This study examines whether the use of more accurate embedding potentials improves the convergence of quantum mechanics/molecular mechanics (QM/MM) models with respect to the size of the QM region. In conjunction with density functional theory calculations using the ωB97X-D functional, various embedding potentials including the TIP3P water model, the effective fragment potential (EFP), and semi-empirical methods (PM6, PM7, and DFTB) were used to simulate the deprotonation energies of solvated acid clusters. The calculations were performed on solvated neutral (HA) and cationic (HB+) acids clusters containing 160 and 480 water molecules using configurations sampled from molecular dynamics simulations. Consistently, the ωB97X-D/EFP model performed the best when using a minimal QM region size. The performance for the other potentials appears to be highly sensitive to the charge character of the acid/base pair. Neutral acids display the expected trend that semi-empirical methods generally perform better than TIP3P; however, an opposite trend was observed for the cationic acids. Additionally, electronic embedding provided an improvement over mechanical embedding for the cationic systems, but not the neutral acids. For the best performing ωB97X-D/EFP model, a QM region containing about 6% of the total number of solvent molecules is needed to approach within 10 kJ mol−1 of the pure QM result if the QM region was chosen based on the distance from the reaction centre.


1978 ◽  
Vol 56 (2) ◽  
pp. 266-279 ◽  
Author(s):  
L. Wilk ◽  
W. R. Fehlner ◽  
S. H. Vosko

The spin-density functional theory was used to calculate the electronic thermal effective masses (including electron–electron interactions) and the spin susceptibilities (via a variational principle) for beryllium and magnesium. The necessary exchange-correlation functionals were treated in the local-spin-density approximation. The single-particle electron states were calculated by the augmented-plane-wave method using a self-consistent muffin-tin potential. It was found that the calculated thermal effective masses agreed very well with semi-empirical results from fits to the Fermi surface. We conclude that the accepted values of the electron–phonon mass enhancement parameter λep are too large by approximately 50%. The theoretical spin susceptibiltiy for Be was found to be 0.47 × 10−6 (cgs volume units), in marked disagreement with the experimental values. For Mg we obtained the value 1.65 × 10−6 (cgs volume units).


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