Abstracts of the CTTC School 2016
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General Introduction
Eduard Matito
Universidad País Vasco
In this course we will introduce a few concepts that will be used in the subsequent four Chemical Bonding courses. We will follow the follow sketch:
- Density and Density Matrices.
- The Atom in a Molecule. Atomic partitions
- The Quantum Theory of Atoms in Molecules (QTAIM) partition. - Mulliken's partition.
- Population Analysis
- Electron Sharing Indices.
Andreas Savin
CNRS and Sorbonne Universités, UPMC Univ Paris 06
Density Functional Theory
- Foundations of density functional theory
- The Hohenberg-Kohn theorem
- Accurate functionals
- Response functions
- Methods used in the frame of density theory
- The Kohn-Sham method
- Functionals for the kinetic, exchange, correlation energies
- Scaling
- Tools for constructing approximations, and extending density functional theory
- Adiabaitc connection
- Hybrids
- Approximations for density functionals
- LDA
- Semi-local approximations
- Hybrids
- Combination with Hartree-Fock
- Combination with multi-reference methods
- Methods for excited states
- Main limitations of approximations
- Systematic improvement
- Treatment of degeneracy and size-consistency
- Methods related to density functional theories
- Local potentials
- Random phase approximation
- Judging approximations
- Concepts from statistics
- Benchmarks and their limits
Tomás Rocha
Univ. Autónoma de México
Summary
José L. Gázquez
Universidad Autónoma Metropolitana-Iztapalapa, México
Chemical reactivity in density functional theory
The Taylor series expansion of the energy as a function of the number of electrons and the external potential, around an isolated chemical species, has been the basis of the density functional theory of chemical reactivity. The response functions that appear through this approach describe the inherent or intrinsic chemical reactivity, which may be used to infer the behavior of a molecule when it interacts with different families of reagents. In this presentation we will revise the concepts that arise from the derivatives of the energy with respect to the number of electrons, basically, the chemical potential and the chemical hardness, and the derivatives of the electronic density with respect to the number of electrons, basically, the Fukui function and the dual descriptor. We will also analyze the chemical potential equalization principle, the maximum hardness principle and the hard and soft acids and bases principle, and their importance to describe chemical interactions. Additionally, we will make use of the Hohenberg-Kohn-Mermin formalism in the grand canonical ensemble to derive the temperature dependent expressions. Finally, we will discuss the charge transfer process from the perspective of density functional theory to show the relevance of the concepts of chemical potential and hardness in chemistry.
Development
Paul Ayers
McMaster Univ.
Summary
Peter Gill
Australian National University
Although density functional theory (DFT) has become extremely popular within the quantum chemistry community, it still suffers from some serious deficiencies and most of these are now well understood. One of the key goals of modern research, therefore, is to develop new methods that preserve the low cost of DFT calculations while offering significantly enhanced accuracy.
Many of the problems of DFT stem from the fact that most functionals are based on the uniform electron gas, a model that consists of an infinite number of electrons in an infinite volume. Unfortunately, this system does not resemble the electron density in most molecules and one route to the improvement of DFT is to replace this foundation with a new one.
Electrons-on-a-sphere is a particularly attractive model because it is defined by a single parameter (the radius R of the sphere) and varying this takes us from a weakly correlated system (small R) dominated by dynamical correlation, to a strongly correlated system (large R) dominated by static correlation.
I will review this model and show how it can be used as the starting point for a new way of understanding and improving DFT.
Miquel Huix-Rotllant
CNRS and Université Aix-Marseille
Time-dependent density functional theory (TDDFT) has become a fundamental tool in quantum chemistry to calculate excited state properties of molecular systems with up to several hundreds of atoms. Despite this success, the approximations performed at the level of the exchange-correlation functional limit its accuracy. Indeed, several important problems have been detected like incorrect description of static correlation, the wrong description of charge-transfer and/or Rydberg states, or the incorrect description of state intersections with the ground state. This course will be divided in two parts: first, I will give a simple introduction to exact TDDFT and the main approximations usually applied to solve TDDFT equations in practice, focusing on the main drawbacks that are frequently encountered in approximate TDDFT. Second, we will do a hands-on tutorial with some practical examples like analysis of excited states and simulation of absorption and emission spectra for some organic molecules.
Cyrus Umrigar
Cornell Univ.
Summary
Materials
Carlos Cárdenas
Universidad de Chile
Summary
Varinia Bernales
Minesotta U.
Summary
Juan E. Peralta
Department of Physics and Science of Advanced Materials Program, Central Michigan University, Mount Pleasant, MI 48859, USA.
Magnetic Properties of Transition Metal Complexes from Density Functional Theory
The characterization of the magnetic properties of molecular systems is important to understand and make predictions of the magnetic behavior of materials where magnetism is of molecular origin.[1] In this short course we will first briefly review the physical origin and theory of magnetic properties in molecular systems, and describe current methods to evaluate these properties in complexes containing transition metal atoms using density functional theory (DFT).[1-4] We will emphasize the strengths and deficiencies of DFT for these properties, including those intrinsic of DFT and those of current approximations. Finally, we will analyze real examples using the magnetic anisotropy energy and magnetic exchange couplings in connection to observed magnetic experimental data. [5-7]
[1] O. Kahn, Molecular Magnetism, VCH: New York, NY (1993).
[2] J. Kortus, M. R. Pederson, T. Baruah, N. Bernstein, and C. S. Hellberg, Density functional studies of single molecule magnets, Polyhedron 22, 1871 (2003).
[3] C. van Wüllen, Magnetic anisotropy from density functional calculations. Comparison of different approaches: Mn12O12 acetate as a test case, J. Chem. Phys. 130, 194109 (2009).
[4] J. J. Phillips, and J. E. Peralta, The role of range-separated Hartree-Fock exchange in the calculation of magnetic exchange couplings in transition metal complexes, J. Chem. Phys. 134 034108 (2011).
[5] Jens Kortus, Tunna Baruah, Noam Bernstein, and Mark R. Pederson, Magnetic ordering, electronic structure, and magnetic anisotropy energy in the high-spin Mn10 single molecule magnet, Phys. Rev. B 66 092403 (2002).
[6] J. J. Phillips, J. E. Peralta, and G. Christou, Magnetic couplings in spin frustrated FeIII7 disklike clusters, J. Chem. Theory Comput. 9, 5585 (2013).
[7] R. P. Joshi, J. J. Phillips, and J. E. Peralta, Magnetic exchange couplings in heterodinuclear complexes based on differential local spin rotations, J. Chem. Theory Comput. 12, 1728 (2016).
Jorge Seminario
Texas A&M University
Theoretical Chemistry Analyses for the Study and Design of Materials for Rechargeable Batteries
A review of the applications of theoretical chemistry methods for the development of new materials for rechargeable batteries will be shown [1-7]. Including, the concerted use of quantum and classical methods such as DFT on one hand and molecular dynamics on the other to solve key problems such as the solid electrolyte interphase formation and the mechanisms of electrode and electrolyte damage due mostly to electron tunneling from the anode to the electrolyte. The field of electrochemistry presents a challenge to engineers and scientists due to the strict multiscale and multidisciplinary nature of the problems. We will start with a rapid description of the methodology and the programs used, followed by their application to key materials and systems, and ending with some important results and describing possibilities for the future.
[1] L. Benitez, D. Cristancho, J. M. Seminario, J. M. Martinez de la Hoz, and P. B. Balbuena,
"Electron transfer through solid-electrolyte-interphase layers formed on Si anodes of Li-ion
batteries," Electrochimica Acta, vol. 140, pp. 250-257, 2014.
[2] S. M. Aguilera-Segura and J. M. Seminario, "Ab Initio Analysis of Silicon Nano-Clusters," J. Phys. Chem. C, vol. 118, pp. 1397-1406, 2014.
[3] F. A. Soto, Y. Ma, J. M. Martinez de la Hoz, J. M. Seminario, and P. B. Balbuena, "Formation and Growth Mechanisms of Solid-Electrolyte Interphase Layers in Rechargeable Batteries," Chem. Mat., vol. 27, pp. 7990-8000, 2015.
[4] Y. Ma, J. M. Martinez de la Hoz, I. Angarita, J. M. Berrio-Sanchez, L. Benitez, J. M. Seminario, et al., "Structure and Reactivity of Alucone-Coated Films on Si and LixSiy Surfaces," ACS Appl. Mater. Interfaces., vol. 7, pp. 11948-11955, 2015.
[5] F. A. Soto, J. M. Martinez de la Hoz, J. M. Seminario, and P. B. Balbuena, "Modeling Solid- Electrolyte Interfacial Phenomena in Silicon Anodes," Current Opinion in Chemical Engineering.
[6] G. Ramos-Sanchez, F. A. Soto, J. M. M. d. l. Hoz, Z. Liu, P. P. Mukherjee, F. El-Mellouhi, et al., "Computational Studies of Interfacial Reactions at Anode Materials: Initial Stages of the Solid-Electrolyte-Interphase Layer Formation," Journal of Electrochemical Energy Conversion and Storage.
[7] N. Kumar and J. M. Seminario, "Lithium-Ion Model Behavior in an Ethylene Carbonate Electrolyte Using Molecular Dynamics," J. Phys. Chem. C, In Press.
Chemical Bonding
Marco García-Revilla
Univ. Guanajuato, México
Summary The study of the Chemical Bond belongs to the most important issues in Chemistry. The new methodologies in this field enable us to rationalize chemical phenomenon where the traditional models fail. The Interacting Quantum Atoms (IQA)[1,2] and the Electron Distribution Functions EDF[3] belong to such new methodologies. IQA and EDF have been shown to be successful to deal with the study of the Chemical Bond. Two studies are presented in this lecture. 1) Oxygen under extreme pressure conditions, the unexplained physicochemical behavior of O2 under pressure can be finally rationalized by the IQA and EDF methodology.[4] 2) Constructing molecular graphs from IQA bonding descriptors, the exchange-correlation energies can be used to draw molecular graphs with physical insight.[5]
[1] A. Martín Pendás, M. A. Blanco, and E. Francisco. J. Chem. Phys. 2004, 120, 4581; J. Comput. Chem. 2005, 26, 344; J. Chem. Theory Comput. 2005,1,1096; J. Comput. Chem. 2007, 28, 16;. A. Martín Pendás, M. A. Blanco, and E. Francisco. J. Chem. Phys. 2006, 125. 184112 A. Martín Pendás, M. A. Blanco,and E. Francisco. J. Comput. Chem. 2009, 30, 98; D. Tiana et al. J. Chem.Theory Comput. 2010, 6, 1064; D. Tiana et. al. Phys. Chem. Chem. Phys. 2011,13, 5068.
[2] A. Martín Pendás, E. Francisco, M. A. Blanco, and Carlo Gatti. Chem. Eur.
J. 13, 9362 (2007).
[3] E. Francisco, A. Martín Pendás, M. A. Blanco. J. Chem. Phys. 126, 094102 (2007); E. Francisco, M. A. Blanco , A. Martín Pendás. Comp. Phys. Commun. 178, 621 (2008); A. Martín Pendás, E. Francisco, M. A. Blanco, Phys. Chem. Chem. Phys. 9, 1087 (2007).
[4] M. A García-Revilla, E.Francisco, A.Martín Pendás, J.M.Recio, M.I.Hernández, J. Campos-Martínez, E. Carmona-Novillo, and R. Hernández-Lamoneda. J. Chem. Theory Comput., 9, 2179 (2013).
[5] M. A García-Revilla, E. Francisco, PL. Popelier, and A. Martín Pendás. Chemphyschem, 14,1211 (2013).
Ángel Martín Pendás
Universidad de Oviedo. Spain.
A real space perspective of how energy and electrons distribute in molecules: Interacting quantum atoms and electron distribution functions
The topological approach to chemical bonding in real space, or Quantum
Chemical Topology (QCT) has now come of age. Its best known flavor, the
Quantum Theory of Atoms in Molecules (QTAIM) [1] has been extremely
successful, providing an orbital invariant theory of chemical bonding problems
based on an observable, the electron density, amenable to experimental
determination. In this course we will consider the basics
of QCT as well as two development that expands its scope and predictive power:
the Interacting Quantum Atoms (IQA) [2-3] approach, which provides an exact
energetic decomposition within the QTAIM valid at general geometries, and the
electron distribution functions (EDF) [4].
[1] R. F. W. Bader, Atoms in Molecules , Oxford University Press., Oxford (1990). [2] A. Martín Pendás, M. A. Blanco, and E. Francisco. J. Chem. Phys. 2004, 120, 4581; J. Comput. Chem. 2005, 26, 344; J. Chem. Theory Comput. 2005, 1, 1096; J. Comput. Chem. 2007, 28, 16;. A. Martín Pendás, M. A. Blanco, and E. Francisco. J. Chem. Phys. 2006, 125. 184112 A. Martín Pendás, M. A. Blanco, and E. Francisco. J. Comput. Chem. 2009, 30, 98; D. Tiana et al. J. Chem. Theory Comput. 2010, 6, 1064; D. Tiana et. al. Phys. Chem. Chem. Phys. 2011, 13, 5068. [3] A. Martín Pendás, E. Francisco, M. A. Blanco, and Carlo Gatti. Chem. Eur. J. 13, 9362 (2007). [4] E. Francisco, A. Martín Pendás, M. A. Blanco. J. Chem. Phys. 126, 094102 (2007); E. Francisco, M. A. Blanco , A. Martín Pendás. Comp. Phys. Commun. 178, 621 (2008); A. Martín Pendás, E. Francisco, M. A. Blanco, Phys. Chem. Chem. Phys. 9, 1087 (2007).
Summary
Eloy Ramos-Cordoba
University of California, Berkeley
Summary
Pedro Salvador
Universitat de Girona
Summary