21 research outputs found

    ASCR/HEP Exascale Requirements Review Report

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    This draft report summarizes and details the findings, results, and recommendations derived from the ASCR/HEP Exascale Requirements Review meeting held in June, 2015. The main conclusions are as follows. 1) Larger, more capable computing and data facilities are needed to support HEP science goals in all three frontiers: Energy, Intensity, and Cosmic. The expected scale of the demand at the 2025 timescale is at least two orders of magnitude -- and in some cases greater -- than that available currently. 2) The growth rate of data produced by simulations is overwhelming the current ability, of both facilities and researchers, to store and analyze it. Additional resources and new techniques for data analysis are urgently needed. 3) Data rates and volumes from HEP experimental facilities are also straining the ability to store and analyze large and complex data volumes. Appropriately configured leadership-class facilities can play a transformational role in enabling scientific discovery from these datasets. 4) A close integration of HPC simulation and data analysis will aid greatly in interpreting results from HEP experiments. Such an integration will minimize data movement and facilitate interdependent workflows. 5) Long-range planning between HEP and ASCR will be required to meet HEP's research needs. To best use ASCR HPC resources the experimental HEP program needs a) an established long-term plan for access to ASCR computational and data resources, b) an ability to map workflows onto HPC resources, c) the ability for ASCR facilities to accommodate workflows run by collaborations that can have thousands of individual members, d) to transition codes to the next-generation HPC platforms that will be available at ASCR facilities, e) to build up and train a workforce capable of developing and using simulations and analysis to support HEP scientific research on next-generation systems.Comment: 77 pages, 13 Figures; draft report, subject to further revisio

    The OpenMolcas Web: A Community-Driven Approach to Advancing Computational Chemistry

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    The developments of the open-source OpenMolcas chemistry software environment since spring 2020 are described, with a focus on novel functionalities accessible in the stable branch of the package or via interfaces with other packages. These developments span a wide range of topics in computational chemistry and are presented in thematic sections: electronic structure theory, electronic spectroscopy simulations, analytic gradients and molecular structure optimizations, ab initio molecular dynamics, and other new features. This report offers an overview of the chemical phenomena and processes OpenMolcas can address, while showing that OpenMolcas is an attractive platform for state-of-the-art atomistic computer simulations

    Free energy evaluation by molecular dynamics simulations. Analysis of a perturbation method and a thermodynamic integrationtechnique

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    Een belangrijke conclusie uit de chemische thermodynamica is dat een verandering in een systeem in thermisch contact met een warmtebad alleen spontaan kan verlopen als de vrije energie van het beschouwde systeem afneemt. Dit maakt de vrije energie een van de belangrijkste thermodynamische grootheden. Met de ontwikkeling van computersimulatietechnieken is ook een aantal methoden voorgesteld om deze grootheid te berekenen. ... Zie: Samenvatting

    Molecular and Dissociative Adsorption of Water on (TiO<sub>2</sub>)<sub><i>n</i></sub> Clusters, <i>n</i> = 1–4

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    The low energy structures of the (TiO<sub>2</sub>)<sub><i>n</i></sub>(H<sub>2</sub>O)<sub><i>m</i></sub> (<i>n</i> ≀ 4, <i>m</i> ≀ 2<i>n</i>) and (TiO<sub>2</sub>)<sub>8</sub>(H<sub>2</sub>O)<sub><i>m</i></sub> (<i>m</i> = 3, 7, 8) clusters were predicted using a global geometry optimization approach, with a number of new lowest energy isomers being found. Water can molecularly or dissociatively adsorb on pure and hydrated TiO<sub>2</sub> clusters. Dissociative adsorption is the dominant reaction for the first two H<sub>2</sub>O adsorption reactions for <i>n</i> = 1, 2, and 4, for the first three H<sub>2</sub>O adsorption reactions for <i>n</i> = 3, and for the first four H<sub>2</sub>O adsorption reactions for <i>n</i> = 8. As more H<sub>2</sub>O’s are added to the hydrated (TiO<sub>2</sub>)<sub><i>n</i></sub> cluster, dissociative adsorption becomes less exothermic as all the Ti centers become 4-coordinate. Two types of bonds can be formed between the molecularly adsorbed water and TiO<sub>2</sub> clusters: a Lewis acid–base Ti–O­(H<sub>2</sub>) bond or an O···H hydrogen bond. The coupled cluster CCSD­(T) results show that at 0 K the H<sub>2</sub>O adsorption energy at a 4-coordinate Ti center is ∌15 kcal/mol for the Lewis acid–base molecular adsorption and ∌7 kcal/mol for the H-bond molecular adsorption, in comparison to that of 8–10 kcal/mol for the dissociative adsorption. The cluster size and geometry independent dehydration reaction energy, <i>E</i><sub>D</sub>, for the general reaction 2­(−TiOH) → −TiOTi– + H<sub>2</sub>O at 4-coordinate Ti centers was estimated from the aggregation reaction of <i>n</i>Ti­(OH)<sub>4</sub> to form the monocyclic ring cluster (TiO<sub>3</sub>H<sub>2</sub>)<sub><i>n</i></sub> + <i>n</i>H<sub>2</sub>O. <i>E</i><sub>D</sub> is estimated to be −8 kcal/mol, showing that intramolecular and intermolecular dehydration reactions are intrinsically thermodynamically allowed for the hydrated (TiO<sub>2</sub>)<sub><i>n</i></sub> clusters with all of the Ti centers 4-coordinate, which can be hindered by cluster geometry changes caused by such processes. Bending force constants for the TiOTi and OTiO bonds are determined to be 7.4 and 56.0 kcal/(mol·rad<sup>2</sup>). Infrared vibrational spectra were calculated using density functional theory, and the new bands appearing upon water adsorption were assigned

    Developments in computer architecture and the birth and growth of computational chemistry

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    It goes almost without saying that the impressive development of computational chemistry in the past 50-60 years is a direct consequence of the even more impressive developments in computer hardware and software in that same period. However, this development also required the vision and skills of pioneering scientists that saw the new possibilities early, such as Roothaan and students at the University of Chicago, Slater’s group at MIT, and the Boys group at Cambridge, United Kingdom. Yet, we might recall in this context that it was a chemical physics problem, the calculation of the dielectric constant of Helium, that inspired John Atanasoff, working on his PhD thesis in Madison, Wisconsin in 1930, to think about designing an electronic calculating machine. About 10 years later, at Ames, Iowa, with the help of his student Clifford Berry, he succeeded in building the first electronic computer-the ABC, the Atanasoff-Berry computer. Because of war circumstances, this invention was never patented and only in October 1973 it was legally settled that the ABC and not the ENIAC was the first electronic computer ever built. A fairly complete account of this interesting episode in computer history can be found on the site www.columbia.edu/∌td2177/JVAtanasoff/JVAtanasoff.html

    Comparison of Computational Strategies for the Calculation of the Electronic Coupling in Intermolecular Energy and Electron Transport Processes

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    Electronic couplings in intermolecular electron and energy transfer processes calculated by six different existing computational techniques are compared to nonorthogonal configuration interaction for fragments (NOCI-F) results. The paper addresses the calculation of the electronic coupling in diketopyrrolopyrol, tetracene, 5,5â€Č-difluoroindigo, and benzene–Cl for hole and electron transport, as well as the local exciton and singlet fission coupling. NOCI-F provides a rigorous computational scheme to calculate these couplings, but its computational cost is rather elevated. The here-considered ab initio Frenkel–Davydov (AIFD), Dimer projection (DIPRO), transition dipole moment coupling, Michl–Smith, effective Hamiltonian, and Mulliken–Hush approaches are computationally less demanding, and the comparison with the NOCI-F results shows that the NOCI-F results in the couplings for hole and electron transport are rather accurately predicted by the more approximate schemes but that the NOCI-F exciton transfer and singlet fission couplings are more difficult to reproduce
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