Molecular properties and basis set quality: An approach based on information theory

Information theory can be used to evaluate the quality of a wave function by considering its ability to give values for some observables as close as possible to the experimental ones. A new method for improving the quality of a wave function is proposed. This paper deals exclusively with the HF (X ¹∑⁺) molecule.     

孪函数N电子基组的组态

分析了各类孪函数Ｎ电子基组态展开式的特点以及它们对体系相关能的贡献,提出了一种在享函数Ｎ电子基矢下进行多组态自洽场计算时的组态选取方法,并依此方法在ＳＴＯ－６－３１Ｇ基组下对ＬｉＨ分子的基态能量做了计算,结果表明,用该组态选取方法只需选取少量的组态波函数便可得到相当精确的计算结果。     

The 6-31G++ basis set: An economical basis set for correlated wavefunctions

The 6-31G ⁺⁺ basis set is described. This basis set is very similar to the existing 6-31G ^** set but is somewhat smaller through the use of five (rather than six) second-order Gaussians (d functions) and has polarization function exponents optimized for correlated rather than Hartree–Fock wavefunctions. The performance of 6-31G ⁺⁺ is compared with that of the 6-31G ^** and 6-31G ^** basis sets through calculation of the geometries and atomization energies for the set of molecules LiH, FH, H₂O, NH₃, CH₄, N₂, CO, HCN, and HCCH.     

Geometrical basis set for molecular computations

To simplify the computation of many center two-electron integrals in large molecules a new type of basis set - called geometrical - is proposed. Its flexibility is tested for atoms from Z = 1 to 38 and for positive and negative ions. This basis is designed mainly for improving large-molecule computations but we have tested it with an accuracte computation for H₂O.     

A correlation-consistent basis set for Fe

 A series of correlation-consistent basis sets are developed for Fe. Our best computed ⁵F–⁵D separation in the Fe atom is in excellent agreement with experiment. Our best estimate for the FeCO D ₀ value is in good agreement with experiment. The ⁵Σ⁻–³Σ⁻ separation in FeCO has an error of 3.6 kcal/mol; while the origin of this error is not clear, it is probably not due to the basis set. Received: 5 March 2001 / Accepted: 2 May 2001 / Published online: 9 August 2001     

Views on quality tests of radiopharmaceuticals

The quality tests of radionuclides produced from generators (⁹⁹Mo→^99mTc,¹¹³Sn→^113mIn) have been reviewed. The quality controls of radiopharmaceuticals derived from these radionuclides and prepared with the help of ready-for-use reagents assembled in kits have been presented. The possibility of new tests regarding sterility (by means of a radiometric method) and detection of endotoxin (based on gelification of limulus amoebocyte lysate) have been suggested.     

Improving numerical integration through basis set expansion

Calculations are presented to assess a theorem presented by S.F. Boys [(1969) Proc. R. Soc. A. 309:195], regarding the accuracy of numerical integration in quantum chemical calculations. The theorem states that the error due to numerical integration can be made proportional to the error due to basis set truncation, and thus goes to zero in the limit of a complete basis. We test this theorem on the hydrogen atom, showing that with a solution-spanning basis, the numerically exact orbital energy can indeed be calculated with a small number of integration points. Moreover, tests for H and H₂⁺ demonstrate that even when only a near-complete basis is employed, Boys Theorem can significantly reduce integration error. However, for other systems, like the oxygen atom and the CO₂ molecule, the theorem yields no advantage for some occupied orbitals. It is concluded that the theorem would be most useful for calculations that demand large basis sets.     

Local orbital eigenvalues and basis set balance

Consideration of the chemical potential of an electron in a wavefunction suggests that a quantity called the local orbital eigenvalue and its variation in space provides a method of testing the balance of a basis set as a function of spatial position. The Hartree-Fock method as applied to the helium and neon atoms is used as an example.     

The 3-21G(N*) basis set: An economical polarized basis set for ab initio studies on nitrogen-containing molecules

The 3-21G basis set shares with its older cousin, the 4-31G basis set, a tendency to overestimate valence angles at nitrogen atoms and to underestimate seriously barriers to inversion at such atoms. The 6-31G* basis set generally yields greatly improved results in these respects. It is here shown that, for a variety of molecules, supplementation of the 3-21G basis set at three- or two-coordinate nitrogen atoms with a set of six d-functions having exponent 1.0 leads to optimized geometries and inversion barriers at such nitrogen centers in good agreement with results obtained with the 6-31G* basis set. This supplemented basis set, designated as 3-21G(N*), also leads to calculated vibrational frequencies in good agreement with those calculated with the 6-31G* basis set. The 3-21G(N*) basis set offers an economical alternative to the 6-31G* basis set, particularly for molecules containing several first-row atoms other than nitrogen.     

Ab initio CI calculations on benzene with an extended basis set

An extended basis set of triple zeta plus polarization quality is employed to carry out configuration interaction (CI ) calculations of the three lowest singlet and triplet excited states of benzene. The CI calculation is carried out by taking into account single and double excitations of π and σ electrons. In the CI , composite natural orbitals (CNO s), which are constructed from the natural orbitals of the ground state of ethylene, are used as virtual orbitals. The aim of using CNOs is to reduce the number of virtual orbitals to be used in constructing configuration-state functions, thus cutting down CI dimensions without losing reasonable accuracy. The excitation energies resulting from the CI are in fairly good agreement with experiment. The root mean square of the deviation is 0.22 eV for the six calculated energies and the largest disagreement is 0.37 eV for the third singlet excited state. To obtain better excitation energies by an ab initio calculation, it seems likely that we need to take into account more electron correlation than in the present calculation. © 1994 John Wiley & Sons, Inc.     

Representation of cusps in a hyperspherical basis set

The wave functions of Coulomb systems have cusps at points corresponding to two particle coelescences. In this paper, we derive series representing the cusps in terms of hyperspherical harmonics multiplied by functions of the hyperradius. When the hyperspherical method is applied to Coulomb systems, the harmonics which appear in these series should be included in the hyperangular basis set.     

Gaussian basis set for molecular wavefunctions containing second-row atoms

A Gaussian basis set consisting of 12s-type and 9p-type functions has been optimized for the second-row atoms. Energy values are also reported for different contractions of this basis set.

---

Zusammenfassung Es wird ein Basissatz von 12s- und 9p-Gaußfunktionen für die Atome der zweiten Periode optimiert. Für verschiedene Kontraktionen dieser Basis werden die Energiewerte angegeben.

---

Résumé On presente un ensemble optimal de fonctions de base gaussiennes pour les atomes de la seconde ligne. Cet ensemble comprend 12 fonctions du type s et 9 fonctions du type p. On etudie egalement l'effet de differentes contractions de cet ensemble sur l'energie totale.

     

Performance of numerical basis set DFT for aluminum clusters

We have investigated and compared the ability of numerical and Gaussian-type basis sets combined with density functional theory (DFT) to accurately describe the geometries, binding energies, and electronic properties of aluminum clusters, Al12XHn (X = Al, Si; n = 0, 1, 2). DFT results are compared against high-level benchmark calculations and experimental data where available. Properties compared include geometries, binding energies, ionization potentials, electron affinities, and HOMO-LUMO gaps. Generally, the PBE functional with the double numerical basis set with polarization (DNP) performs very well against experiment and the analytical basis sets for considerably less computational expense.     

Ab initio molecular dynamics with dual basis set methods

On-the-fly, ab initio classical molecular dynamics are demonstrated with an underlying dual basis set potential energy surface. Dual-basis self-consistent field (Hartree-Fock and density functional theory) and resolution-of-the-identity second-order M?ller-Plesset perturbation theory (RI-MP2) dynamics are tested for small systems, including the water dimer. The resulting dynamics are shown to be faithful representations of their single-basis analogues for individual trajectories, as well as vibrational spectra. Computational cost savings of 58% are demonstrated for SCF methods, even relative to Fock-extrapolated dynamics, and savings are further increased to 71% with RI-MP2. Notably, these timings outperform an idealized estimate of extended-Lagrangian molecular dynamics. The method is subsequently demonstrated on the vibrational absorption spectrum of two NO(+)(H?O)? isomers and is shown to recover the significant width of the shared-proton bands observed experimentally.     

Geometry optimizations with a small contracted gaussian basis set

The STO-2G basis set has been used to calculate equilibrium geometries of 27 molecules. A comparison with STO-3G and experimental results indicates that the exploration of potential energy surfaces of large organic molecules can be efficiently carried out using the STO-2G basis set.     

Localized basis orbitals: minimization of 2-electron integrals array and orthonormality of basis set

A new scheme for deriving localized basis orbitals (LBOs) and for obtaining integral transformations from the basis orbitals (BOs) to the LBOs has been introduced. The scheme was tested at the ab initio Hartree-Fock level using the STO-3G basis set. It has been revealed that it provides results that are close to the conventional ab initio approximations for various physical-chemical properties. At the same time, both the number of differential overlaps and the number of electron repulsion integrals (ERIs) grow with the system size notably slower than those calculated for the usual BOs. The power exponent for ERI/LBO is typically smaller by 0.3-0.6 than that for ERI/BO. The exponent reaches the value of 1.69 even for triglycine (24 atoms only), which represents a relatively small molecular model. Thus, the localization of the BOs (using LBOs) may result in additional improvements in efficiency even for electronically delocalized systems. It was shown that ERI/LBO is particularly efficient for systems with complex spatial structures (including conjugated species). The obtained results indicate that the proposed scheme could be included in computational methods targeted at calculating large molecular systems (which achieve linear scaling for more distant interactions). Neglecting ERI/LBO does not depend on the delocalization of the localized MO using ERI/LBO. The orthogonality and locality of the LBOs should make them useful in methods based on dividing the system into orthogonal subsystems.     

The effect of basis set superposition error on the convergence of interaction energies

 For the intermolecular interaction energies of ion-water clusters [OH⁻(H₂O) _n (n=1,2), F⁻(H₂O), Cl⁻(H₂O), H₃O⁺(H₂O) _n (n=1,2), and NH₄ ⁺(H₂O) _n (n=1,2)] calculated with correlation-consistent basis sets at MP2, MP4, QCISD(T), and CCSD(T) levels, the basis set superposition error is nearly zero in the complete basis set (CBS) limit. That is, the counterpoise-uncorrected intermolecular interaction energies are nearly equal to the counterpoise-corrected intermolecular interaction energies in the CBS limit. When the basis set is smaller, the counterpoise-uncorrected intermolecular interaction energies are more reliable than the counterpoise-corrected intermolecular interaction energies. The counterpoise-uncorrected intermolecular interaction energies evaluated using the MP2/aug-cc-pVDZ level is reliable. Received: 14 March 2001 / Accepted: 25 April 2001 / Published online: 9 August 2001