Academia.edu no longer supports Internet Explorer.
To browse Academia.edu and the wider internet faster and more securely, please take a few seconds to upgrade your browser.
1997, Journal of Physical Chemistry A
An efficient route to the site-selective reactivity of electronically excited states of multicentered molecules is discussed. In the first stage the migration of the electronic excitation occurs. This can operate over an extensive range without extensive draining of energy into the nuclear frame. Only in a second stage, once the optimal site has been reached, does the excess energy become available for bond breaking or isomerization at the new, optimal, site. This two-stage mechanism, where electronic excitation (or the charge) is the scout, avoids the pitfall of conventional large molecule kinetics. (In that view, known as the quasi equilibrium theory, the electronic excitation is first converted to nuclear modes. But then there are so many available vibrational states that the probability for the excitation energy to become localized at the necessary site is too small and the resulting reaction rate is too slow.) By confining the site search to the electronic manifold, it becomes a highly efficient process. The recent novel experiments of Weinkauf et al. on (positive) charge migration and dissociation of peptide ions are suggested as an example of the considerations above where there is a facile migration of the positive charge followed by reactivity at the selected site. The peptide is modeled as beads on a chain. Interbead and intrabead coupling are discussed in terms of adiabatic and diabatic states. We find a multistep mechanism (unlike superexchange): a charge-directed reactivity (CDR) model. Such efficient ranging could also take place in other chain structures and suggests that there will be examples where electronic processes set the time scale for the chemical change.
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
Theory and Applications of Computational Chemistry, 2005
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.
The Journal of Chemical Physics, 2007
A recently introduced computational algorithm to extend time scales of atomically detailed simulations is illustrated. The algorithm, Milestoning, is based on partitioning the dynamics to a sequence of trajectories between "milestones" and constructing a non-Markovian model for the motion along a reaction coordinate. The kinetics of a conformational transition in a blocked alanine is computed and shown to be accurate, more efficient than straightforward Molecular Dynamics by a factor of about 9, and nonexponential. A general scaling argument predicts linear speed-up with the number of milestones for diffusive processes, and exponential speed-up for transitions over barriers. The algorithm is also trivial to parallelize. As a side result Milestoning also produces the free energy profile along the reaction coordinate, and is able to describe non-equilibrium motions along one (or a few) degrees of freedom.
Chemical Reviews, 2009
The Journal of Physical Chemistry A, 1999
In this paper, we give a full account of our studies of the dynamics of electron-transfer reactions. We examine bimolecular reactions of various donors and acceptors and focus on the reversible and dissociative elementary steps probed directly using femtosecond time, speed, and angular resolutions. In particular, we report studies of the bimolecular systems of the following electron donors: diethyl sulfide, p-dioxane, acetone, and benzene. The electron acceptors are iodine and iodine monochloride. The general phenomena of reversible and dissociative electron transfer are found for all systems studied. The dynamics of the dative bonding, from the transition state (TS) to final products, involve two elementary processes with different reaction times, speed and angular distributions. For example, for the diethyl sulfide‚iodine system, it is shown that after charge separation, the entire complex is trapped in the TS region and the reversible electron transfer occurs in less than 500 femtosecond (lifetime), followed by the rupture of the I-I bond with the release of the first exterior I-atom. However, the second process of the remaining and trapped (caged) interior I-atom takes 1.15 ps with its speed (500 m/s) being much smaller than the first one (1030 m/s). The initial structure is determined to be a nearly linear configuration of S-I-I (165°), consistent with the ab inito calculations and predictions of the HOMO-LUMO frontier orbitals. The observed time scales and bifurcation of the wave packet, with different speeds, are illustrated on the global potential energy surface with the help of molecular dynamics simulations. The findings on this and the other systems reported here elucidate the mechanism and address the concepts of nonconcertedness, caging, and restricted energy dissipation, which are important to the description of reaction mechanisms in the condensed phase, on surfaces, and in electrochemical studies.
Science, 2007
Ion imaging reveals distinct photodissociation dynamics for propanal cations initially prepared in either the cis or gauche conformation, even though these isomers differ only slightly in energy and face a small interconversion barrier. The product kinetic energy distributions for the hydrogen atom elimination channels are bimodal, and the two peaks are readily assigned to propanoyl cation or hydroxyallyl cation coproducts. Ab initio multiple spawning dynamical calculations suggest that distinct ultrafast dynamics in the excited state deposit each conformer in isolated regions of the ground-state potential energy surface, and, from these distinct regions, conformer interconversion does not effectively compete with dissociation.
Electronic excitations along sites that undergo spatial and temporal fluctuations due to conformational chain motion have been studied in the picture of the stochastic master equation by means of the dynamic Monte Carlo ~DMC! and the cumulant expansion ~CE! approach. An incoherent site-to-site hopping which is adiabatic relative to the changes of conformational site coordinates has been assumed. The elementary act of conformational change has been considered to be fast, whereas the electronic transfer during the time period of the conformational event has been assumed to be negligibly small. The time evolution of electronic intersite coupling is thus controlled by chromophore sites that, in particular, correspond to the conformational minima of the potential energy landscape. The generalized equations of motion adapted for both the DMC and the CE analysis have been reduced to formulate donor site excitation probabilities ^Pi exc(t)& and donor excitation survival functions ^PD(t)& for a simplified chain. In this polymer model, ~i! specific nearest-neighbor electronic coupling occurs with two distinct transfer rates W1 and W2 corresponding to two different spatial arrangements of the pendant sites in the pair and ~ii! transitions between two definite conformational states occur both in the correlated and in the uncorrelated regime. For short chains and a moderate number of sites in the rotational dyads the whole range from the dynamic to the static limit in the interplay between excitation transfer and correlated conformational motion has been calculated by the DMC method. By means of the cumulant technique well-behaved solutions could be obtained only in the fast conformational transition regime which allows a direct comparison with the DMC results. For longer chains up to 100 sites, in the limit case of uncorrelated conformational motion, preliminary cumulant approaches have been given which, for very rapid conformational rates, agree well with the dynamic effective medium approximation ~DEMA solutions.
Journal of the American Chemical Society, 2011
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.
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.
Chemical Science, 2010
A variety of chemical phenomena are governed by non-adiabatic transitions at conical intersections of potential energy surfaces, if not directly, but indirectly in the midst of the processes. In other words, the non-adiabatic transition makes one of the most significant key mechanisms in chemical dynamics. Since the basic analytical theory is now available to treat the transitions, it is possible to comprehend the dynamics of realistic chemical and biological systems with the effects of transitions taken into account properly. Another important quantum mechanical effect of tunneling can also be taken into account. Furthermore, it becomes feasible to control chemical dynamics by controlling the non-adiabatic transitions at conical intersections, and also to develop new molecular functions by using peculiar properties of non-adiabatic transitions. These may be realized, if we apply appropriately designed laser fields. This perspective review article explains the above mentioned ideas based on the authors' recent activities. The non-adiabatic chemical dynamics is expected to open a new dimension of chemistry.
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?
Chemical Reviews, 2006
Damien Riedel received his B.Sc. in physics from the University of Besanc ¸on. His M.Sc. work in optics and electronics was on speckle interferometry using a scanning near-field optical microscope in the Laboratoire d'Optique P. M. Duffieux. He obtained his Ph.D. in physics in 1998 under the supervision of Prof. M. C. Castex from the University of Paris XIII, where his postgraduate work in laser physics and surface science concerned the vacuum ultraviolet laser interaction with polymer surfaces and fluorescence spectroscopy. He then joined the group of Prof. R. E. Palmer in Birmingham, U.K., on a postdoctoral Marie-Curie Fellowship. In the Nanoscale Physics Laboratory, he worked on an ultrashort-pulse laser created by high-order harmonic generation in rare gases. He developed applications on surface photodesorption experiments and room temperature STM combined with a laser. In 2001, he joined the CNRS to work with Dr. Ge ´rald Dujardin, and his research deals with molecular electronics and molecular manipulation via highly localized electronic excitation with a low-temperature STM on semiconductors. He is developing projects that combine a laser and an STM and involve collection of fluorescence on the low-temperature STM.
Advanced Series in Physical Chemistry, 2011
Biophysical Journal, 2014
When structures that interconvert on a given time scale are lumped together, the corresponding free-energy surface becomes af u n c t i o no ft h eo b s e r v a t i o nt i m e .T h i sv i e wi se q u i v a l e n tt o grouping structures that are connected by free-energy barriers below a certain threshold. We illustrate this time dependence for some benchmark systems, namely atomic clusters and alanine dipeptide, highlighting the connections to broken ergodicity, local equilibrium, and "feasible" symmetry operations of the molecular Hamiltonian.
The Journal of Physical Chemistry, 1993
The electronic superexchange interactions, which enable long-range electron transfer in complex molecular structures, such as proteins, are beyond the capacity of standard electronic structure methods due to their size, inhomogeneity, aperiodicity, and sensitivity to the many weak interactions between the nominally insulating atoms of the intervening medium. The inhomogeneous aperiodic lattice theory, presented here, is a novel strategy implemented as a quantum molecular model, designed to enable the calculation of electronic transfer matrix elements in large macromolecular systems by redesigning the electronic structure problem into a twotiered approach. The procedure is (i) assembly of the diagonal and off-diagonal elements of the Hamiltonian matrix by comparison, respectively, with experimental ionization potentials for individual amino acids and with triple-cab initio studies of resonance integrals and then (ii) nonperturbative computation of the macromolecular electronic coupling from this inhomogeneous aperiodic lattice (IAL) Hamiltonian. The IAL method includes all the occupied orbitals of the entire protein in a full-matrix calculation with no a priori assumption about pathways or spatial subregions important in spanning the distance between the redox sites. The nonperturbative approach and overall strategy of subunit-level calibration, distinct from standard semiempirical atom-level calibration, are first presented. A specific algorithm for Hamiltonian construction and tests against a series of medium sized molecules then follow. This nonperturbative matrix inversion strategy is computationally efficient and can treat a system the size of cytochrome c in less than a minute. Most important to the mechanistic study of redox proteins, the absolute results in cm-l for the computed charge resonance energies of three ruthenium modified cytochrome c derivatives compare well with experiment. k,, = (2a/h)lA12(FCWD) Thus the rate constant k, depends upon the product of two factors, lA)* and FCWD, arising, respectively, from the participation of the electronic and nuclear motions in the kinetic process. The Franck-Condon weighted density of final vibronic states, FCWD, is the quantum analogue of the activation factor in the original Marcus rate expression, which describes and predicts the dependence of the rate upon the reorganization free energy and reaction e~ergonicity.1~ This factor is treated quantum mechanically, semiclassically, or in the classical limit as appropriate to the degree of vibrational excitationl"18 and need not be considered
Chemical Physics, 2016
The simulation of nonadiabatic dynamics in extended molecular systems involving hundreds of atoms and large densities of states is particularly challenging. Nonadiabatic coupling terms (NACTs) represent a significant numerical bottleneck in surface hopping approaches. Rather than using unreliable NACT cutting schemes, here we develop "on-the-fly" state limiting methods to eliminate states that are no longer essential for the non-radiative relaxation dynamics as a trajectory proceeds. We propose a state number criteria and an energy-based state limit. The latter is more physically relevant by requiring a user-imposed energy threshold. For this purpose, we introduce a local kinetic energy gauge by summing contributions from atoms within the spatial localization of the electronic wavefunction to define the energy available for upward hops. The proposed state limiting schemes are implemented within the nonadiabatic excited-state molecular dynamics framework to simulate photoinduced relaxation in poly-phenylene vinylene (PPV) and branched poly-phenylene ethynylene (PPE) oligomers for benchmark evaluation.
Loading Preview
Sorry, preview is currently unavailable. You can download the paper by clicking the button above.