2015
DOI: 10.1063/1.4921959
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Transition state theory approach to polymer escape from a one dimensional potential well

Abstract: The rate of escape of an ideal bead-spring polymer in a symmetric double-well potential is calculated using transition state theory (TST) and the results compared with direct dynamical simulations. The minimum energy path of the transitions becomes flat and the dynamics diffusive for long polymers making the Kramers-Langer estimate poor. However, TST with dynamical corrections based on short time trajectories started at the transition state gives rate constant estimates that agree within a factor of two with t… Show more

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Cited by 7 publications
(13 citation statements)
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“…The transition state theory approach followed by explicit dynamical corrections is then preferable over Kramers' approach. Similar at barrier issues arise in polymer escape problems where HTST followed by recrossing corrections has been shown to be a useful approach for estimating the transition rate. 13 At low enough temperature, quantum tunneling through the energy barrier becomes the dominant transition mechanism and the rate can eventually become temperature independent. It is important to have a way to estimate the crossover temperature for tunneling when assessing the stability of a magnetic state.…”
Section: Introductionmentioning
confidence: 99%
“…The transition state theory approach followed by explicit dynamical corrections is then preferable over Kramers' approach. Similar at barrier issues arise in polymer escape problems where HTST followed by recrossing corrections has been shown to be a useful approach for estimating the transition rate. 13 At low enough temperature, quantum tunneling through the energy barrier becomes the dominant transition mechanism and the rate can eventually become temperature independent. It is important to have a way to estimate the crossover temperature for tunneling when assessing the stability of a magnetic state.…”
Section: Introductionmentioning
confidence: 99%
“…A detailed analysis of the eigenmodes, the barrier height, the barrier shape, and the removal of the peak has been presented in our previous publication. 36 The HTST estimate of the rate saturates to a constant value in the region N > 32. This is because the height of the effective energy barrier, the maximum along the MEP, saturates as the barrier starts to flatten out as shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…(9). Anharmonic corrections 36,25 are computed for this mode but they do not completely remove the peak. A detailed analysis of the eigenmodes, the barrier height, the barrier shape, and the removal of the peak has been presented in our previous publication.…”
Section: Resultsmentioning
confidence: 99%
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