D. Van Neck

Variational determination of the second-order density matrix for the isoelectronic series of beryllium, neon, and silicon

B. Verstichel, H. van Aggelen, D. Van Neck, P.W. Ayers, P. Bultinck
Physical Review A
80 (3), 032508
2009
A1

Abstract 

The isoelectronic series of Be, Ne and Si are investigated using a variational determination of the second-order density matrix. A semidefinite program was developed that exploits all rotational and spin symmetries in the atomic system. We find that the method is capable of describing the strong static electron correlations due to the incipient degeneracy in the hydrogenic spectrum for increasing central charge. Apart from the ground-state energy various other properties are extracted from the variationally determined second-order density matrix. The ionization energy is constructed using the extended Koopmans' theorem. The natural occupations are also studied, as well as the correlated Hartree-Fock-like single particle energies. The exploitation of symmetry allows to study the basis set dependence and results are presented for correlation-consistent polarized valence double, triple and quadruple zeta basis sets.

Open Access version available at UGent repository

Incorrect diatomic dissociation in variational reduced density matrix theory arises from the flawed description of fractionally charged atoms

H. van Aggelen, P. Bultinck, B. Verstichel, D. Van Neck, P.W. Ayers
Physical Chemistry Chemical Physics (PCCP)
11 (27), 5558-5560
2009
A1

Abstract 

The behaviour of diatomic molecules is examined using the variational second-order density matrix method under the P, Q and G conditions. It is found that the method describes the dissociation limit incorrectly, with fractional charges on the well-separated atoms. This can be traced back to the behaviour of the energy versus the number of electrons for the isolated atoms. It is shown that the energies for fractional charges are much too low.

Exact ionization potentials from wavefunction asymptotics: The extended Koopmans’ theorem, revisited

D. Vanfleteren, D. Van Neck, P.W. Ayers, R.C. Morrison, P. Bultinck
Journal of Chemical Physics
130 (19), 194104
2009
A1

Abstract 

A simple explanation is given for the exactness of the extended Koopmans’ theorem, (EKT) for computing the removal energy of any many-electron system to the lowest-energy ground state ion of a given symmetry. In particular, by removing the electron from a “removal orbital” of appropriate symmetry that is concentrated in the asymptotic region, one obtains the exact ionization potential and the exact Dyson orbital for the corresponding state of the ion. It is argued that the EKT is not restricted to many-electron systems but holds for any finite many-body system, provided that the interaction vanishes for increasing interparticle distance. A necessary and sufficient condition for the validity of the EKT for any state (not just the lowest-energy states of a given symmetry) in terms of the third-order reduced density matrix is stated and derived.

Comparison of the Hirshfeld-I and iterated stockholder atoms in molecules schemes

P. Bultinck, D.L. Cooper, D. Van Neck
Physical Chemistry Chemical Physics (PCCP)
11 (18), 3424-3429
2009
A1

Abstract 

Two recently introduced self-consistent Hirshfeld procedures for obtaining atoms in molecules are compared in detail. The Hirshfeld-I scheme introduces self consistency by requiring that the atomic population of the promolecular atom is equal to that of the atom-in-the-molecule. In the iterated stockholder atoms (ISA) approach, self consistency is obtained by requiring that for every value of the radius of a sphere around every nucleus, the average electron density on the surface of this sphere is the same in the promolecular atom and in the atom in the molecule. The relationships between the two schemes are examined, and common backgrounds and differences are discussed. Whereas it can be argued that the Hirshfeld-I approach has a stronger physical background, the ISA scheme avoids having to define what states of the atoms are to be considered when constructing the promolecule.

Early stages of α-α′ phase separation in Fe-Cr alloys: An atomistic study

G. Bonny, D. Terentyev, L. Malerba, D. Van Neck
Physical Review B
79 (10), 104207
2009
A1

Abstract 

The thermal aging of Fe-Cr alloys was simulated using atomistic kinetic Monte Carlo techniques. The study was performed varying the Cr content in the range of 12–18 at. % Cr and at temperatures within the miscibility gap, where α-α′ phase separation occurs. The evolution of the phase-separation process was characterized in terms of precipitate shape, composition, density, and mean size. The results offer a description of α-α′ phase separation in its early stage, which is hardly accessible to experiments and of key importance in understanding the change in mechanical properties of Fe-Cr alloys under thermal aging. The critical size for a stable precipitate was estimated from the simulation data in the framework of Gibbs's homogeneous nucleation theory. The obtained results are compared, whenever possible, with available experimental data and the reliability, as well as the shortcomings, of the applied method is discussed accordingly. Despite strong oversimplifications, the used model shows good agreement with experimental data.

Normal modes for large molecules with arbitrary link constraints in the mobile block Hessian approach

A. Ghysels, D. Van Neck, B.R. Brooks, V. Van Speybroeck, M. Waroquier
Journal of Chemical Physics
130 (8), 084107
2009
A1

Abstract 

In a previous paper [ Ghysels et al., J. Chem. Phys. 126, 224102 (2007) ] the mobile block Hessian (MBH) approach was presented. The method was designed to accurately compute vibrational modes of partially optimized molecular structures. The key concept was the introduction of several blocks of atoms, which can move as rigid bodies with respect to a local, fully optimized subsystem. The choice of the blocks was restricted in the sense that none of them could be connected, and also linear blocks were not taken into consideration. In this paper an extended version of the MBH method is presented that is generally applicable and allows blocks to be adjoined by one or two common atoms. This extension to all possible block partitions of the molecule provides a structural flexibility varying from very rigid to extremely relaxed. The general MBH method is very well suited to study selected normal modes of large macromolecules (such as proteins and polymers) because the number of degrees of freedom can be greatly reduced while still keeping the essential motions of the molecular system. The reduction in the number of degrees of freedom due to the block linkages is imposed here directly using a constraint method, in contrast to restraint methods where stiff harmonic couplings are introduced to restrain the relative motion of the blocks. The computational cost of this constraint method is less than that of an implementation using a restraint method. This is illustrated for the α-helix conformation of an alanine-20-polypeptide. © 2009 American Institute of Physics

Mobile Block Hessian Approach with Adjoined Blocks: An Efficient Approach for the Calculation of Frequencies in Macromolecules

A. Ghysels, V. Van Speybroeck, E. Pauwels, D. Van Neck, B.R. Brooks, M. Waroquier
Journal of Chemical Theory and Computation (JCTC)
5 (5), 1203-1215
2009
A1

Abstract 

In an earlier work, the authors developed a new method, the mobile block Hessian (MBH) approach, to accurately calculate vibrational modes for partially optimized molecular structures [ J. Chem. Phys. 2007, 126 (22), 224102.]. It is based on the introduction of blocks, consisting of groups of atoms, that can move as rigid bodies. The internal geometry of the blocks need not correspond to an overall optimization state of the total molecular structure. The standard MBH approach considers free blocks with six degrees of freedom. In the extended MBH approach introduced herein, the blocks can be connected by one or two adjoining atoms, which further reduces the number of degrees of freedom. The new approach paves the way for the normal-mode analysis of biomolecules such as proteins. It rests on the hypothesis that low-frequency modes of proteins can be described as pure rigid-body motions of blocks of consecutive amino acid residues. The method is validated for a series of small molecules and further applied to alanine dipeptide as a prototype to describe vibrational interactions between two peptide units; to crambin, a small protein with 46 amino acid residues; and to ICE/caspase-1, which contains 518 amino acid residues.

Ab-initio Green's Functions Calculations of Atoms

C. Barbieri, D. Van Neck
AIP Conference Proceedings
1120, 104-108
2009
A1

Abstract 

The Faddeev random phase approximation (FRPA) method is applied to calculate the ground state and ionization energies of simple atoms. First ionization energies agree with the experiment at the level of ~10 mH or less. Calculations with similar accuracy are expected to provide information required for developing the proposed quasiparticle-DFT method. ©2009 American Institute of Physics

Calculating Reaction Rates with Partial Hessians: Validation of the Mobile Block Hessian Approach

A. Ghysels, V. Van Speybroeck, T. Verstraelen, D. Van Neck, M. Waroquier
Journal of Chemical Theory and Computation (JCTC)
4 (4) 614-625
2008
A1

Abstract 

In an earlier paper, the authors have developed a new method, the mobile block Hessian (MBH), to accurately calculate vibrational modes for partially optimized molecular structures [J. Chem. Phys. 2007, 126 (22), 224102]. The proposed procedure remedies the artifact of imaginary frequencies, occurring in standard frequency calculations, when parts of the molecular system are optimized at different levels of theory. Frequencies are an essential ingredient in predicting reaction rate coefficients due to their input in the vibrational partition functions. The question arises whether the MBH method is able to describe the chemical reaction kinetics in an accurate way in large molecular systems where a full quantum chemical treatment at a reasonably high level of theory is unfeasible due to computational constraints. In this work, such a validation is tested in depth. The MBH method opens a lot of perspectives in predicting accurate kinetic parameters in chemical reactions where the standard full Hessian procedure fails.

Cartesian formulation of the mobile block Hessian approach to vibrational analysis in partially optimized systems

A. Ghysels, D. Van Neck, M. Waroquier
Journal of Chemical Physics
127 (16), 164108
2007
A1

Abstract 

Partial optimization is a useful technique to reduce the computational load in simulations of extended systems. In such nonequilibrium structures, the accurate calculation of localized vibrational modes can be troublesome, since the standard normal mode analysis becomes inappropriate. In a previous paper [ A. Ghysels et al., J. Chem. Phys. 126, 224102 (2007) ], the mobile block Hessian (MBH) approach was presented to deal with the vibrational analysis in partially optimized systems. In the MBH model, the nonoptimized regions of the system are represented by one or several blocks, which can move as rigid bodies with respect to the atoms of the optimized region. In this way unphysical imaginary frequencies are avoided and the translational/rotational invariance of the potential energy surface is fully respected. In this paper we focus on issues concerning the practical numerical implementation of the MBH model. The MBH normal mode equations are worked out for several coordinate choices. The introduction of a consistent group-theoretical notation facilitates the treatment of both the case of a single block and the case of multiple blocks. Special attention is paid to the formulation in terms of Cartesian variables, in order to provide a link with the standard output of common molecular modeling programs.

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