Chemical dynamics between wells across a time-dependent barrier: Self-similarity in the Lagrangian descriptor and reactive basins.

In chemical or physical reaction dynamics, it is essential to distinguish precisely between reactants and products for all times. This task is especially demanding in time-dependent or driven systems because therein the dividing surface (DS) between these states often exhibits a nontrivial time-dependence. The so-called transition state (TS) trajectory has been seen to define a DS which is free of recrossings in a large number of one-dimensional reactions across time-dependent barriers and thus, allows one to determine exact reaction rates. A fundamental challenge to applying this method is the construction of the TS trajectory itself. The minimization of Lagrangian descriptors (LDs) provides a general and powerful scheme to obtain that trajectory even when perturbation theory fails. Both approaches encounter possible breakdowns when the overall potential is bounded, admitting the possibility of returns to the barrier long after the trajectories have reached the product or reactant wells. Such global dynamics cannot be captured by perturbation theory. Meanwhile, in the LD-DS approach, it leads to the emergence of additional local minima which make it difficult to extract the optimal branch associated with the desired TS trajectory. In this work, we illustrate this behavior for a time-dependent double-well potential revealing a self-similar structure of the LD, and we demonstrate how the reflections and side-minima can be addressed by an appropriate modification of the LD associated with the direct rate across the barrier.

[1]  S. Wiggins,et al.  The geometry of reaction dynamics , 2002 .

[2]  R. Hernandez,et al.  Deconstructing field-induced ketene isomerization through Lagrangian descriptors. , 2016, Physical chemistry chemical physics : PCCP.

[3]  Carolina Mendoza,et al.  Hidden geometry of ocean flows. , 2010, Physical review letters.

[4]  Thomas Bartsch,et al.  Identifying reactive trajectories using a moving transition state. , 2006, The Journal of chemical physics.

[5]  E. Pollak,et al.  Classical transition state theory is exact if the transition state is unique , 1979 .

[6]  Jaffe,et al.  Transition state theory without time-reversal symmetry: chaotic ionization of the hydrogen atom , 2000, Physical review letters.

[7]  B. Sussman,et al.  Dynamic Stark Control of Photochemical Processes , 2006, Science.

[8]  H. Waalkens,et al.  Reaction dynamics through kinetic transition states. , 2013, Physical review letters.

[9]  S. Keshavamurthy,et al.  Local phase space control and interplay of classical and quantum effects in dissociation of a driven Morse oscillator , 2008, 0809.3062.

[10]  Chemical reactions induced by oscillating external fields in weak thermal environments. , 2015, The Journal of chemical physics.

[11]  Thomas Bartsch,et al.  Transition state in a noisy environment. , 2005, Physical review letters.

[12]  E. Pollak,et al.  Transition states, trapped trajectories, and classical bound states embedded in the continuum , 1978 .

[13]  Shinnosuke Kawai,et al.  A New Look at the Transition State: Wigner's Dynamical Perspective Revisited , 2005 .

[14]  Stochastic transition states: reaction geometry amidst noise. , 2005, The Journal of chemical physics.

[15]  C. Jaffé,et al.  Classical S‐matrix theory for chaotic atom–diatom collisions , 1994 .

[16]  Donald G. Truhlar,et al.  Multidimensional transition state theory and the validity of Grote-Hynes theory , 2000 .

[17]  T. Komatsuzaki,et al.  Dynamic pathways to mediate reactions buried in thermal fluctuations. I. Time-dependent normal form theory for multidimensional Langevin equation. , 2009, The Journal of chemical physics.

[18]  R. Hernandez,et al.  Lagrangian Descriptors of Thermalized Transition States on Time-Varying Energy Surfaces. , 2015, Physical review letters.

[19]  T Uzer,et al.  Statistical theory of asteroid escape rates. , 2002, Physical review letters.

[20]  Rigoberto Hernandez,et al.  Transition state theory in liquids beyond planar dividing surfaces , 2010 .

[21]  T. Bartsch,et al.  Persistence of transition-state structure in chemical reactions driven by fields oscillating in time. , 2014, Physical review. E, Statistical, nonlinear, and soft matter physics.

[22]  W. Thompson,et al.  Removing the barrier to the calculation of activation energies. , 2016, The Journal of chemical physics.

[23]  B. C. Garrett,et al.  Current status of transition-state theory , 1983 .

[24]  T. Komatsuzaki,et al.  Quantum reaction boundary to mediate reactions in laser fields. , 2011, The Journal of chemical physics.

[25]  R. Hernandez,et al.  Uncovering the Geometry of Barrierless Reactions Using Lagrangian Descriptors. , 2016, The journal of physical chemistry. B.

[26]  W. Miller,et al.  Semiclassical transition state theory. A new perspective , 1993 .

[27]  Shane D. Ross,et al.  Heteroclinic connections between periodic orbits and resonance transitions in celestial mechanics. , 2000, Chaos.

[28]  R. Hernandez A combined use of perturbation theory and diagonalization: Application to bound energy levels and semiclassical rate theory , 1994 .

[29]  Chun-Biu Li,et al.  Definability of no-return transition states in the high-energy regime above the reaction threshold. , 2006, Physical review letters.

[30]  Chemical reaction dynamics within anisotropic solvents in time-dependent fields. , 2005, The Journal of chemical physics.

[31]  Kaoru Yamanouchi,et al.  The Next Frontier , 2002, Science.

[32]  Donald G. Truhlar,et al.  Generalized transition state theory. Classical mechanical theory and applications to collinear reactions of hydrogen molecules , 1979 .

[33]  R. Berry,et al.  Dynamical hierarchy in transition states: Why and how does a system climb over the mountain? , 2001, Proceedings of the National Academy of Sciences of the United States of America.

[34]  C. Jaffé,et al.  Chaotic scattering: An invariant fractal tiling of phase space , 1995 .

[35]  T. Bartsch,et al.  Communication: Transition state trajectory stability determines barrier crossing rates in chemical reactions induced by time-dependent oscillating fields. , 2014, The Journal of chemical physics.

[36]  Jeremy M Moix,et al.  Time‐Dependent Transition State Theory , 2008 .

[37]  B. C. Garrett,et al.  The definition of reaction coordinates for reaction‐path dynamics , 1991 .

[38]  T Uzer,et al.  Transition state theory for laser-driven reactions. , 2007, The Journal of chemical physics.

[39]  Stephen Wiggins,et al.  Lagrangian descriptors: A method for revealing phase space structures of general time dependent dynamical systems , 2011, Commun. Nonlinear Sci. Numer. Simul..

[40]  T. Komatsuzaki,et al.  Robust existence of a reaction boundary to separate the fate of a chemical reaction. , 2010, Physical review letters.

[41]  G. Henkelman,et al.  Analytic dynamical corrections to transition state theory , 2016 .

[42]  S. Keshavamurthy,et al.  Classical-quantum correspondence in a model for conformational dynamics: Connecting phase space reactive islands with rare events sampling , 2015 .

[43]  R. M. Benito,et al.  Transition state geometry of driven chemical reactions on time-dependent double-well potentials. , 2016, Physical chemistry chemical physics : PCCP.

[44]  Michael Baer,et al.  Theory of chemical reaction dynamics , 1985 .

[45]  P. Pechukas,et al.  TRANSITION STATE THEORY , 1981 .

[46]  T. Komatsuzaki,et al.  Dynamical switching of a reaction coordinate to carry the system through to a different product state at high energies. , 2011, Physical review letters.