Erratum: “Nonexponentiality of time dependent survival probability and the fractional viscosity dependence of the rate in diffusion controlled reactions in a polymer chain” [J. Chem. Phys. 114, 9170 (2001)]

2001 ◽  
Vol 115 (13) ◽  
pp. 6268-6268 ◽  
Author(s):  
Goundla Srinivas ◽  
Arun Yethiraj ◽  
Biman Bagchi
Keyword(s):  
Polymer Chain ◽  
Survival Probability ◽  
Chem Phys ◽  
Time Dependent ◽  
Diffusion Controlled ◽  
Viscosity Dependence

Diffusion controlled reactions: Experimental verification of the time‐dependent rate equation

1988 ◽  
Vol 89 (8) ◽  
pp. 4799-4806 ◽  
Author(s):  
N. Periasamy ◽  
S. Doraiswamy ◽  
B. Venkataraman ◽  
G. R. Fleming
Keyword(s):  
Rate Equation ◽  
Experimental Verification ◽  
Time Dependent ◽  
Dependent Rate ◽  
Diffusion Controlled

Length and Time-Dependent Rates in Diffusion-Controlled Reactions with Conjugated Polymers

2009 ◽  
Vol 113 (12) ◽  
pp. 2786-2795 ◽  
Author(s):  
Paiboon Sreearunothai ◽  
Sadayuki Asaoka ◽  
Andrew R. Cook ◽  
John R. Miller
Keyword(s):  
Conjugated Polymers ◽  
Time Dependent ◽  
Diffusion Controlled

RESONANCES IN H+HLi SCATTERING FOR NONZERO TOTAL ANGULAR MOMENTUM (J > 0): A TIME-DEPENDENT WAVE PACKET APPROACH

2006 ◽  
Vol 05 (04) ◽  
pp. 871-885 ◽  
Author(s):  
R. PADMANABAN ◽  
S. MAHAPATRA
Keyword(s):  
Angular Momentum ◽  
Wave Packet ◽  
Total Angular Momentum ◽  
Energy Surface ◽  
Chem Phys ◽  
Time Dependent ◽  
Coriolis Coupling ◽  
Initial State ◽  
Sudden Approximation ◽  
Franck Condon

The resonances in H + HLi scattering for nonzero total angular momentum (J > 0) are examined here by a time-dependent wave packet approach employing an ab initio potential energy surface (PES) [Dunne LJ, Murrell JN, Jemmer P, Chem Phys Lett336: 1, 2001] of the system. The resonances are identified by calculating a set of pseudospectra corresponding to the Franck–Condon transition of a hypothetical initial state to the interaction region of the H + HLi PES. The resonances are characterized by calculating their eigenfunctions and linewidth lifetimes. The resonances for J ≠ 0 are discussed in relation to their counterpart for J = 0. The effect of Coriolis coupling on the resonances obtained from the centrifugal sudden approximation for J = 2 and for K = 0,1,2 is examined.

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