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2005, Theory and Applications of Computational Chemistry
In this paper we present a time-dependent, direct, nonadiabatic theory of molecular processes. We put this approach in contrast to the current theory paradigm of approximate separation of electronic and nuclear dynamics, which proceeds via approximate electronic stationary states and corresponding potential energy surfaces. This established approach in all its variants has provided a basis for qualitative understanding of rate processes and, for systems with few nuclear degrees of freedom, it has produced quantitative data that can be used to guide experiments. In this picture the dynamics of the reacting system takes place on a stationary electronic state potential surface and may under the influence of nonadiabatic coupling terms "jump" to another potential surface the probability of such transitions often viewed as a statistical "surface hopping" [ J. Chem. Phys., 55 (1971) 562] event. The time-dependent, direct, and nonadiabatic theory presented here is fully dynamical in that the evolving state, which describes the simultaneous dynamics of electrons and nuclei of a reacting system [Rev. Mod. Phys., 66(3), (1994) 917] changes in time under the mutual instantaneous forces in a Cartesian laboratory system of coordinates. This approach, which has been applied to reactive collisions involving polyatomic molecules over a large range of energies, proceeds without predetermined potential energy surfaces, uses total molecular wave functions that are parameterized as generalized coherent states, and imposes no constraints on molecular geometries.
Annual review of physical chemistry, 1998
To predict the branching between energetically allowed product channels, chemists often rely on statistical transition state theories or exact quantum scattering calculations on a single adiabatic potential energy surface. The potential energy surface gives the energetic barriers to each chemical reaction and allows prediction of the reaction rates. Yet, chemical reactions evolve on a single potential energy surface only if, in simple terms, the electronic wavefunction can evolve from the reactant electronic configuration to the product electronic configuration on a time scale that is fast compared to the nuclear dynamics through the transition state. The experiments reviewed here investigate how the breakdown of the Born-Oppenheimer approximation at a barrier along an adiabatic reaction coordinate can alter the dynamics of and the expected branching between molecular dissociation pathways. The work reviewed focuses on three questions that have come to the forefront with recent theory and experiments: Which classes of chemical reactions evidence dramatic nonadiabatic behavior that influences the branching between energetically allowed reaction pathways? How do the intramolecular distance and orientation between the electronic orbitals involved influence the nonadiabaticity in the reaction? How can the detailed nuclear dynamics mediate the effective nonadiabatic coupling encountered in a chemical reaction?
Faraday discussions, 2014
Gas-phase scattering analysis, data analysis Addendum The referenced proposal builds on our past studies, L560, to explore the imaging of chemical dynamics with ultrafast time resolution and atomic scale molecular structure resolution. It makes the case that it will be possible to create a molecular movie that reveals just how the molecular structure changes, in real time, as the molecule undergoes a chemical reaction.
The Journal of Physical Chemistry, 1996
An approach which allows for multi-electronic-state dynamics but which is in the spirit of classical molecular dynamics is discussed and applied to both collisional ("curve crossing") and ultrafast optical excitation problems. The formalism seeks to allow for the possibility of quite different nuclear dynamics (e.g., bound vs dissociative) in the different electronic states. The discussion begins from a wave function formulation of the problem, and this enables one to retain interference effects if these are important, but the ultimate objective is to obtain as classical-like a description as possible while taking account of the inter-electronic state coupling. The essential approximation in the method is in the computation of these coupling terms which appear as nonclassical corrections to the classical equations of motion. The computational results are tested against accurate quantal computations, and the agreement is typically quantitative.
Journal of Mathematical Chemistry, 2005
The method discussed in this work provides a theoretical framework where simple chemical reactions resemble any other standard quantum process, i.e., a transition in quantum state mediated by the electromagnetic field. In our approach, quantum states are represented as a superposition of electronic diabatic basis functions, whose amplitudes can be modulated by the field and by the external control of nuclear configurations. Using a one-dimensional three-state model system, we show how chemical structure and dynamics can be represented in terms of these control parameters, and propose an algorithm to compute the reaction probabilities. Our analysis of effective energy barriers generalizes previous ideas on structural similarity between reactant, and product, and transition states using the geometry of conventional reaction paths. In the present context, exceptions to empirical rules such as the Hammond postulate appear as effects induced by the environment that supplies the external field acting on the quantum system.
The Journal of Chemical Physics, 1984
Molecular beam and spectroscopic techniques allow detailed study of many dynamical properties of single reactive collisions. The chemical scope of these methods is now very wide and includes certain unimolecular and termolecular reactions as well as bimolecular reactions and energy transfer processes. Results for more than 50 families of A + BC-AB + C atom transfer reactions reveal simple impulsive and persistent complex regimes that correlate with electronic structure. Recent work has found examples of AB + CD-+ AD + BC and AB + CD + EF-AF + BC + DE reactions that require exchange of two or three pairs of bonds in a single collision event yet proceed with practically no activation energy. Processes akin to liquid phase reactions are also becoming accessible to dynamical studies using beams of van der Waals polymers or solvation clusters.
Advanced Series in Physical Chemistry, 2011
Chemical Reviews
The Born-Oppenheimer approximation underlies much of chemical simulation and provides the framework defining the potential energy surfaces that are used for much of our pictorial understanding of chemical phenomena. However, this approximation breaks down when considering the dynamics of molecules in excited electronic states. Describing dynamics when the Born-Oppenheimer approximation breaks down requires a quantum mechanical description of the nuclei. Chemical reaction dynamics on excited electronic states is critical for many applications in renewable energy, chemical synthesis, and bioimaging. Furthermore, it is necessary in order to connect with many ultrafast pump-probe spectroscopic experiments. In this review, we provide an overview of methods that can describe nonadiabatic dynamics with emphasis on those that are able to simultaneously address the quantum mechanics of both electrons and nuclei. Such ab initio quantum molecular dynamics methods solve the electronic Schrödinger equation alongside the nuclear dynamics and thereby avoid the need for precalculation of potential energy surfaces and nonadiabatic coupling matrix elements. Two main families of methods are commonly employed to simulate nonadiabatic dynamics in molecules: full quantum dynamics such as the multiconfigurational time-dependent Hartree method and classical trajectory-based approaches such as trajectory surface hopping. In this review, we describe a third class of methods that is intermediate between the two-Gaussian basis set expansions built around trajectories.
The following papers were published or submitted for publication: Large Amplitude Vibrational Motion in a One Dimensional Chain-Coherent State Representation; Spectroscopic Properties of Polyenes III-1, 3, 5, 7- Octatetraene; On Vibrational Population Relaxation in Solution; Internal Energy Transfer in Isolated Molecules: Ergodic and Nonergodic Behavior-In Proceedings of a Symposium on Advances in Laser Chemistry; The Influence of Nonrandom Sequential Coupling on Radiationless Relaxation Processes; Rotational Effects in Radiationless Processes in Polyatomic Molecules; Single Vibronic Level Fluorescence From Aniline; Collision Induced Intramolecular Vibrational Energy Transfer in 1B2 Aniline; A Numerical Study of Large Amplitude Motion on a Chain of Coupled Nonlinear Oscillators; Angular Momentum Constraints in Radiationless Processes: The Symmetric Top Molecule; Low Energy Collisional Relaxation of 1(2) * in He: Evidence for Resonance Enhanced Vibrational Deactivation; Dynamics of R...
The Journal of Chemical Physics, 2012
Radiationless transitions between electronic excited states in polyatomic molecules take place through unavoided crossings of the potential energy surfaces with substantial non-adiabatic coupling between the respective adiabatic states. While the extent in time of these couplings are large enough, these transitions can be reasonably well simulated through quantum transitions using trajectory surface hopping-like methods. In addition, complex molecular systems may have multiple "trivial" unavoided crossings between noninteracting states. In these cases, the non-adiabatic couplings are described as sharp peaks strongly localized in time. Therefore, their modeling is commonly subjected to the identification of regions close to the particular instantaneous nuclear configurations for which the energy surfaces actually cross each other. Here, we present a novel procedure to identify and treat these regions of unavoided crossings between non-interacting states using the so-called Min-Cost algorithm. The method differentiates between unavoided crossings between interacting states (simulated by quantum hops), and trivial unavoided crossings between non-interacting states (detected by tracking the states in time with Min-Cost procedure). We discuss its implementation within our recently developed non-adiabatic excited state molecular dynamics framework. Fragments of two-and four-ring linear polyphenylene ethynylene chromophore units at various separations have been used as a representative molecular system to test the algorithm. Our results enable us to distinguish and analyze the main features of these different types of radiationless transitions the molecular system undertakes during internal conversion.
International Journal of Quantum Chemistry, 1994
The content of an ab-inddo time-dependent theory of quantm molecular dynamics of electrons and atomic nuclei is presented. Employing the time-dependent variational principle and a family of approximate state vectors yields a set of dynamical equations approximating the time-dependent SchrOdinger equation. These equations govern the time evolution of the relevant state vector parameters as molecular orbital coefficients, nuclear positions and momenta. This approach does not impose the Born-Oppenheimer approximation, does not use potential energy a. surfaces and takes into account elecow-nuclear coupling. Basic cnservation laws are fully ' obeyed. The simplest model of the theory employs a single determinantal state for the electrons CL and classical nuclei and is implemented in the computer code ENDyne. Results from this ab-. _ kio theory are reported for ion-atom and ion-molecule collisions.
Reviews of Modern Physics, 1994
An overview is presented of methods for time-dependent treatments of molecules as systems of electrons and nuclei. The theoretical details of these methods are reviewed and contrasted in the light of a recently developed time-dependent method called electron-nuclear dynamics. Electron-nuclear dynamics (END) is a formulation of the complete dynamics of electrons and nuclei of a molecular system that eliminates the necessity of constructing potential-energy surfaces. Because of its general formulation, it encompasses many aspects found in other formulations and can serve as a didactic device for clarifying many of the principles and approximations relevant in time-dependent treatments of molecular systems. The END equations are derived from the time-dependent variational principle applied to a chosen family of efhciently parametrized approximate state vectors. A detailed analysis of the END equations is given for the case of a single-determinantal state for the electrons and a classical treatment of the nuclei. The approach leads to a simple formulation of the fully nonlinear time-dependent Hartree-Fock theory including nuclear dynamics. The nonlinear END equations with the ab initio Coulomb Hamiltonian have been implemented at this level of theory in a computer program, ENDyne, and have been shown feasible for the study of small molecular systems. Implementation of the Austin Model 1 semiempirical Hamiltonian is discussed as a route to large molecular systems. The linearized END equations at this level of theory are shown to lead to the random-phase approximation for the coupled system of electrons and nuclei. The qualitative features of the general nonlinear solution are analyzed using the results of the linearized equa-918 918 920 920 921 921 922 922 922 923 923 923 923 924 924 925 925 926 928 928 928 929 929 930 931 931 933 935 935 937 937 937 940 941 atomic orbitals nal basis of trav-B. Nonorthogonal representation 1. Derivation in an orthonormal basis a. Metric b. Density matrix c. Energy 2. Derivation in the atomic-orbital basis a. Definition of parameters b. Dynamic orbitals c. Metric d. Density matrix e. Energy 3. Details of semiempirical approaches References 950 950 959
Chemical Physics, 2003
A reactive flux correlation function formalism for the calculation of rate constants for mixed quantum-classical systems undergoing nonadiabatic dynamics is presented. The linear response formalism accounts for the stationarity of the equilibrium density under quantum-classical dynamics and expresses the rate constant in terms of an ensemble of surface-hopping trajectories. Calculations are carried out on a model two-level system coupled to a nonlinear oscillator which is in turn coupled to a harmonic heat bath. Relevant microscopic species variables for this system include two stable states, corresponding to the ground state adiabatic surface, as well as another species corresponding to the excited state surface. The time-dependent rate constants for the model are evaluated in the adiabatic limit, where the dynamics is confined to the ground Born-Oppenheimer surface, and these results are compared with calculations that account for nonadiabatic transitions among the system states.
Physical Review A, 1989
The time-dependent description of the dynamics of electron-molecule collision complexes is out- lined within the framework of Feshbach's projection-operator formalism. It is shown that the equation of motion for the quantum-mechanical wave packet representing the collision complex contains effective-potential terms which are nonlocal as well as non-Markovian, that is, the time develop- rnent depends on the previous history of the system. The space-time integro-differential equation of motion is explicitly (numerically) solved for a class of simple models using expansions into complete sets of functions in both space and time. The exact wave-packet dynamics is compared with the re- sults obtained in the local-complex-potential approximation, which corresponds to the Markovian approximation for the decay dynamics. The concepts and numerical methods are illustrated for a model of the well-known 'll, , shape resonance in electron-N, scattering, where the boomerang effect is reproduced. For a model of a p-wave shape resonance near threshold, novel qualitative effects are revealed, namely, nonmonotonic electronic decay (recapture of electrorls from the continuum) as well as strong frictional effects i» the vibrational motion. The time-dependent description of virtual-state threshold effects in s-wave scattering is also briefly considered.
2008
Ab inito molecular dynamics, although still challenge, is becoming an available tool for the investigation of the photodynamics of aromatic heterocyclic systems. Potential energy surfaces and dynamics simulations for three particular examples and different aspects of the excited and ground state dynamics are presented and discussed. Aminopyrimidine is investigated as a model for adenine. It shows ultrafast S 1 -S 0 decay in about 400 fs. The inclusion of mass-restrictions to emulate the imidizole group increases the lifetime to about 950 fs, a value similar to the lifetime of adenine. The S 2 -S 1 deactivation, typical in the fast component of the decay of nucleobases, is investigated in pyridone. In this case, the S 2 -state lifetime is 52 fs. The hot ground-state dynamics of pyrrole starting at the puckered conical intersection is shown to produce ring-opened structures consistent with the experimental results
Accounts of Chemical Research - ACCOUNT CHEM RES, 2006
Electronically nonadiabatic or non-Born-Oppenheimer (non-BO) chemical processes (photodissociation, charge-transfer, etc.) in- volve a nonradiative change in the electronic state of the system. Molecular dynamics simulations typically treat nuclei as moving classically on a single adiabatic potential energy surface, and these techniques are not immediately generalizable to non-BO systems due to the inherently quantum mechanical nature of electronic transitions. Here we generalize the concept of a single-surface molecular dynamics trajectory to that of a coupled-surface non- BO trajectory that evolves "semiclassically" under the influence of two or more electronic states and their couplings. Five non-BO trajectory methods are discussed. Next, we summarize the results of a series of systematic studies using a database of accurate quantum mechanical reaction probabilities and internal energy distributions for several six-dimensional model bimolecular scat- tering collisions. ...
Journal of Physics: Conference Series, 2015
Faraday Discussions, 2004
Recent progress in the theoretical treatment of electronically nonadiabatic processes is discussed. First we discuss the generalized Born-Oppenheimer approximation, which identifies a subset of strongly coupled states, and the relative advantages and disadvantages of adiabatic and diabatic representations of the coupled surfaces and their interactions are considered. Ab initio diabatic representations that do not require tracking geometric phases or calculating singular nonadiabatic nuclear momentum coupling will be presented as one promising approach for characterizing the coupled electronic states of polyatomic photochemical systems. Such representations can be accomplished by methods based on functionals of the adiabatic electronic density matrix and the identification of reference orbitals for use in an overlap criterion. Next, four approaches to calculating or modeling electronically nonadiabatic dynamics are discussed: (1) accurate quantum mechanical scattering calculations, (2) approximate wave packet methods, (3) surface hopping, and (4) self-consistent-potential semiclassical approaches. The last two of these are particularly useful for polyatomic photochemistry, and recent refinements of these approaches will be discussed. For example, considerable progress has been achieved in making the surface hopping method more applicable to the study of systems with weakly coupled electronic states. This includes introducing uncertainty principle considerations to alleviate the problem of classically forbidden surface hops and the development of an efficient sampling algorithm for low-probability events. A topic whose central importance in a number of quantum mechanical fields is becoming more widely appreciated is the introduction of decoherence into the quantal degrees of freedom to account for the effect of the classical treatment on the other degrees of freedom, and we discuss how the introduction of such decoherence into a self-consistent-potential approximation leads to a reasonably accurate but very practical trajectory method for electronically nonadiabatic processes. Finally, the performances of several dynamical methods for Landau-Zener-type and Rosen-Zener-Demkov-type reactive scattering problems are compared. 1 Introduction Electronically nonadiabatic processes (also called non-Born-Oppenheimer or non-BO processes) are defined as those in which the electronic state changes nonradiatively during the dynamical event. Electronically nonadiabatic processes are essential parts of visible and ultraviolet photochemistry, collisions of electronically excited species, chemiluminescent reactions, and many recombination reactions, heterolytic dissociations, and electron transfer processes. Often electronic
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