TL;DR: In this paper, the unpolarized absorption and circular dichroism spectra of the fundamental vibrational transitions of the chiral molecule, 4-methyl-2-oxetanone, are calculated ab initio using DFT, MP2, and SCF methodologies and a 5S4P2D/3S2P (TZ2P) basis set.
Abstract: : The unpolarized absorption and circular dichroism spectra of the fundamental vibrational transitions of the chiral molecule, 4-methyl-2-oxetanone, are calculated ab initio. Harmonic force fields are obtained using Density Functional Theory (DFT), MP2, and SCF methodologies and a 5S4P2D/3S2P (TZ2P) basis set. DFT calculations use the Local Spin Density Approximation (LSDA), BLYP, and Becke3LYP (B3LYP) density functionals. Mid-IR spectra predicted using LSDA, BLYP, and B3LYP force fields are of significantly different quality, the B3LYP force field yielding spectra in clearly superior, and overall excellent, agreement with experiment. The MP2 force field yields spectra in slightly worse agreement with experiment than the B3LYP force field. The SCF force field yields spectra in poor agreement with experiment.The basis set dependence of B3LYP force fields is also explored: the 6-31G* and TZ2P basis sets give very similar results while the 3-21G basis set yields spectra in substantially worse agreements with experiment. jg
TL;DR: A force field based on both microscopic and macroscopic data is derived, which combines accuracy with transferability to other polymorphs and the possibility of parametrizing other elements is demonstrated.
Abstract: We address the problem of finding interatomic force fields for silicas from ab initio calculations on small clusters. It is shown that the force field cannot be determined from cluster data alone; incorporation of bulk-system information into the force field remains essential. Bearing this in mind, we derive a force field based on both microscopic (ab initio) and macroscopic (experimental) data. This force field combines accuracy with transferability to other polymorphs. The possibility of parametrizing other elements is also demonstrated.
TL;DR: In this paper, the Navier-Stokes equations permit the presence of an externally imposed body force that may vary in space and time, and the velocity is used to iteratively determine the desired value.
TL;DR: In this paper, a general theory of the forces on singularities in a Hookean elastic continuum is developed, where the singularity is taken to be any state of internal stress satisfying the equilibrium equations but not the compatibility conditions.
Abstract: The parallel between the classical theory of elasticity and the modern physical theory of the solid state is incomplete; the former has nothing analogous to the concept of the force acting on an imperfection (dislocation, foreign atom, etc.) in a stressed crystal lattice. To remedy this a general theory of the forces on singularities in a Hookean elastic continuum is developed. The singularity is taken to be any state of internal stress satisfying the equilibrium equations but not the compatibility conditions. The force on a singularity can be given as an integral over a surface enclosing it. The integral contains the elastic field quantities which would surround the singularity in an infinite medium, multiplied by the difference between these quantities and those actually present. The expression for the force is thus of essentially the same form whether the force is due to applied surface tractions, other singularities or the presence of the free surface of the body (‘image force’). A region of inhomogeneity in the elastic constants modifies the stress field; if it is mobile one can define and calculate the force on it. The total force on the singularities and inhomogeneities inside a surface can be expressed in terms of the integral of a ‘ Maxwell tensor of elasticity’ taken over the surface. Possible extensions to the dynamical case are discussed,
TL;DR: A guided tour of modern charge density analysis can be found in this article, where the authors provide an overview of charge density and its applications in materials and energy science. But the authors do not discuss the application of experimental charge density in bio-molecular reactions.
Abstract: A guided tour through modern charge density analysis.- Electron densities and related properties from the ab-initio simulation of crystalline solids.- Modeling and analysing thermal motion in experimental charge density studies.- Spin and the Complementary Worlds of Electron Position and Momentum Densities.- Past, present and future of charge density and density matrix refinements.- Using wavefunctions to get more information out of diffraction experiments.- Local Models for Joint Position and Momentum Density Studies.- Magnetization densities in material science.- Beyond Standard Charge Density Topological Analyses.- On the Interplay Between Real and Reciprocal Space Properties.- Intermolecular interaction energies from experimental charge density studies.- Chemical Information from Charge Density Studies.- Charge density in materials and energy science.- A generic force field based on Quantum Chemical Topology.- Frontier Applications of Experimental Charge Density and Electrostatics to Bio-Macromolecules.- Charge densities and crystal engineering.- Electron Density Topology of Crystalline Solids at High Pressure.- Bonding changes along solid-solid phase transitions using the Electron Localization Function approach.- Multi-temperature electron density studies.- Transient Charge Density Maps from Femtosecond X-Ray Diffraction.- Charge density and chemical reactions: a unified view from Conceptual DFT.