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. 2014 May;4(3):269-284.
doi: 10.1002/wcms.1172.

The Dalton quantum chemistry program system

Kestutis Aidas  1 Celestino Angeli  2 Keld L Bak  3 Vebjørn Bakken  4 Radovan Bast  5 Linus Boman  6 Ove Christiansen  7 Renzo Cimiraglia  2 Sonia Coriani  8 Pål Dahle  9 Erik K Dalskov  10 Ulf Ekström  11 Thomas Enevoldsen  12 Janus J Eriksen  7 Patrick Ettenhuber  7 Berta Fernández  13 Lara Ferrighi  14 Heike Fliegl  11 Luca Frediani  14 Kasper Hald  15 Asger Halkier  16 Christof Hättig  17 Hanne Heiberg  18 Trygve Helgaker  11 Alf Christian Hennum  19 Hinne Hettema  20 Eirik Hjertenæs  21 Stinne Høst  22 Ida-Marie Høyvik  7 Maria Francesca Iozzi  23 Branislav Jansík  24 Hans Jørgen Aa Jensen  12 Dan Jonsson  25 Poul Jørgensen  7 Joanna Kauczor  26 Sheela Kirpekar  27 Thomas Kjærgaard  7 Wim Klopper  28 Stefan Knecht  29 Rika Kobayashi  30 Henrik Koch  21 Jacob Kongsted  12 Andreas Krapp  31 Kasper Kristensen  7 Andrea Ligabue  32 Ola B Lutnæs  33 Juan I Melo  34 Kurt V Mikkelsen  35 Rolf H Myhre  21 Christian Neiss  36 Christian B Nielsen  37 Patrick Norman  26 Jeppe Olsen  7 Jógvan Magnus H Olsen  12 Anders Osted  38 Martin J Packer  12 Filip Pawlowski  39 Thomas B Pedersen  11 Patricio F Provasi  40 Simen Reine  11 Zilvinas Rinkevicius  41 Torgeir A Ruden  42 Kenneth Ruud  14 Vladimir V Rybkin  28 Pawel Sałek  43 Claire C M Samson  28 Alfredo Sánchez de Merás  44 Trond Saue  45 Stephan P A Sauer  35 Bernd Schimmelpfennig  46 Kristian Sneskov  47 Arnfinn H Steindal  14 Kristian O Sylvester-Hvid  48 Peter R Taylor  49 Andrew M Teale  50 Erik I Tellgren  11 David P Tew  51 Andreas J Thorvaldsen  7 Lea Thøgersen  52 Olav Vahtras  5 Mark A Watson  53 David J D Wilson  54 Marcin Ziolkowski  55 Hans Agren  5
Affiliations
Free PMC article

The Dalton quantum chemistry program system

Kestutis Aidas et al. Wiley Interdiscip Rev Comput Mol Sci. 2014 May.
Free PMC article

Abstract

Dalton is a powerful general-purpose program system for the study of molecular electronic structure at the Hartree-Fock, Kohn-Sham, multiconfigurational self-consistent-field, Møller-Plesset, configuration-interaction, and coupled-cluster levels of theory. Apart from the total energy, a wide variety of molecular properties may be calculated using these electronic-structure models. Molecular gradients and Hessians are available for geometry optimizations, molecular dynamics, and vibrational studies, whereas magnetic resonance and optical activity can be studied in a gauge-origin-invariant manner. Frequency-dependent molecular properties can be calculated using linear, quadratic, and cubic response theory. A large number of singlet and triplet perturbation operators are available for the study of one-, two-, and three-photon processes. Environmental effects may be included using various dielectric-medium and quantum-mechanics/molecular-mechanics models. Large molecules may be studied using linear-scaling and massively parallel algorithms. Dalton is distributed at no cost from http://www.daltonprogram.org for a number of UNIX platforms.

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Figures

FIGURE 1
FIGURE 1
The absolute value of the indirect spin–spin coupling constants (Hz, greater than 0.1 Hz) in valinomycin (left), on a logarithmic scale as a function of the internuclear distance (pm). We have used blue, black, red, and green for the CH, CC, CO, and CN coupling constants, respectively. The spin–spin coupling constants have been calculated at the LDA/6-31G level of theory. (Reproduced with permission from Ref 54. Copyright 2004, John Wiley & Sons, Ltd.)
FIGURE 2
FIGURE 2
Near-edge X-ray absorption fine structure (NEXAFS) study of Gd acetate nanoparticles. The experimental spectrum (top) is compared with the sum of the theoretical spectra (black) for isolated acetate (green) and a coordination complex (red). (Reproduced with permission from Ref 105. Copyright 2012, Springer.)
FIGURE 3
FIGURE 3
One- and two-photon absorption spectra for channelrhodopsin calculated using the polarizable embedding method implemented in Dalton. The insert on the top of the right hand side shows the protein embedding potential projected onto the molecular surface.
FIGURE 4
FIGURE 4
Left: The titin-I27 domain highlighting the disulfide bridging bond and a schematic representation of the stretching of the polyprotein strain by the aid of the atomic force microscopy; right: the titin-I27SS model, designed to model the redox-active site in the titin-I27 domain.
FIGURE 5
FIGURE 5
MP2 study of insulin (787 atoms) in the cc-pVDZ basis (7,604 orbitals). Left: Localized orbitals obtained by minimizing the second power of the orbital variances. The least local occupied (blue) and least local virtual (red) orbitals are plotted using orbital contour values of 0.01 a.u. Right: MP2 electrostatic potential calculated using the DEC scheme plotted on an isodensity surface (0.001 a.u.). The values are indicated by the color box (a.u.).

References

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