2005
DOI: 10.1103/physrevlett.95.058301
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Transition State in a Noisy Environment

Abstract: Transition state theory overestimates reaction rates in solution because conventional dividing surfaces between reagents and products are crossed many times by the same reactive trajectory. We describe a recipe for constructing a time-dependent dividing surface free of such recrossings in the presence of noise. The no-recrossing limit of transition state theory thus becomes generally available for the description of reactions in a fluctuating environment.

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Cited by 85 publications
(132 citation statements)
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References 31 publications
(30 reference statements)
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“…16 The shift (19) and (20) to the TS trajectory as a time-dependent origin is described by the generating function…”
Section: F (T) → 0 As T → ±∞ It Is Clear From (28) That S [µ F ](T)mentioning
confidence: 99%
See 1 more Smart Citation
“…16 The shift (19) and (20) to the TS trajectory as a time-dependent origin is described by the generating function…”
Section: F (T) → 0 As T → ±∞ It Is Clear From (28) That S [µ F ](T)mentioning
confidence: 99%
“…Recent work by Bartsch et al [19][20][21] on TST for time-dependent problems has addressed the inclusion of stochastic time-dependent forces (due to solvents in liquid phase reactions, for example). Starting from the Langevin equation of motion, they showed the existence of a "transition state trajectory," which stays in the vicinity of the barrier for all time.…”
Section: Introductionmentioning
confidence: 99%
“…[24][25][26][27] Unstable POs are of importance in the field of classical reaction dynamics in classical systems where they form recrossingfree dividing surfaces. 2,3, 11,[28][29][30] They are important for understanding tunneling dynamics through a barrier in quantum mechanical reactions wherein the PO on the inverted potential, −V , is the instanton trajectory providing the leading contribution to the path integral. 31 In common between all of these cases, is the invariance of POs as they provide a scaffold from which to obtain other geometric structures, and thus remain objects of current interest such as in, e.g., Refs.…”
Section: Introductionmentioning
confidence: 99%
“…For example, in the context of chemical reaction dynamics, LCPT has been applied to seeking (locally-)no-return transition state and the associated reaction coordinate buried in the phase space for many-degrees of freedom Hamiltonian systems such as intramolecular proton transfer in malonaldehyde [37,38], argon cluster isomerization [30][31][32][33][34][35][36], O( 1 D) + N 2 O → NO + NO [39], a hydrogen atom in crossed electric and magnetic fields [29,40], HCN isomerization [41,42,1,2], and so forth. LCPT was generalized to dissipative systems such as multidimensional (generalized) Langevin formulation to describe reactions under thermal fluctuation, in which no-return transition state can be obtained by incorporating nonlinearity of the system and interactions with heat bath [43][44][45][46][47][48][49][50]. The pioneering studies on semiclassical analog of LCPT was also carried out in late 1980s for multidimensional resonant, nonresonant, and nearly resonant systems [51][52][53]: They presented a method for deriving corrections in powers of Planck's constant by the reflection of the underlying (near) divergence properties of classical chaos, which was found to be effective even at low order corrections in improving the accuracy of the energy eigenvalues.…”
Section: Introductionmentioning
confidence: 99%