2015
DOI: 10.1016/j.bbapap.2015.04.021
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Review of computer simulations of isotope effects on biochemical reactions: From the Bigeleisen equation to Feynman's path integral

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Cited by 19 publications
(15 citation statements)
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References 122 publications
(205 reference statements)
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“…Comparison of these values with those determined from computation for different mechanisms is frequently sufficient to establish the catalytic mechanism. Indeed, as computational methods have improved, experimentally determined kinetic isotope effects have come to provide necessary constraints on the structures of transition state structures derived from computation [3, 4]. …”
mentioning
confidence: 99%
“…Comparison of these values with those determined from computation for different mechanisms is frequently sufficient to establish the catalytic mechanism. Indeed, as computational methods have improved, experimentally determined kinetic isotope effects have come to provide necessary constraints on the structures of transition state structures derived from computation [3, 4]. …”
mentioning
confidence: 99%
“…For instance, its normal kinetic-isotope-effect (KIE) value (which is always larger than unity in the classical world) agrees with the analytical results from the famous Bigeleisen equation (for computing quantum KIE) at the classical limit. [3,21,54,[94][95][96][97][98][99][100][101]…”
Section: Transition-state Theory (Tst) For a Many-body Systemmentioning
confidence: 99%
“…The main source of KIEs in chemical reactions are the vibrational contributions and quantum tunneling effects (as mentioned above we restrict the review to KIEs related to hydrogen atom isotopes). Neglecting tunneling, the Bigeleisen equation has likely been the most widely used method to determine the KIE just using harmonic vibrational frequencies: K I E = k l k h = () υ l * υ h * () i = 1 3 N 7 υ i , l υ i , h () i = 1 3 N 6 υ i , h υ i , l () i = 1 3 N 7 sinh u i , h sinh u i , l () i = 1 3 N 6 sinh u i , l sinh u i , h where the subscripts l and h stand for the light and heavy isotopes, respectively, k l and k h are the respective rate constants, υ l * υ h * is the ratio of the imaginary frequencies at the transition state structure, N is the number of atoms of the supermolecule, υ i is the i th normal mode frequency of the corresponding isotopolog ( l or h ), ‡ denote the transition state structure, u i 0.25em = 0.25em h υ i 2 k B T , k B is Boltzmann's constant, T is temperature, and h is Planck's constant. Equation includes both the zero‐point energy contributions (which are usually the most important vibrational contributions) and the effect caused by the vibrational excited states.…”
Section: The Bigeleisen Equationmentioning
confidence: 99%
“…The Bigeleisen equation can be extended beyond the harmonic vibrational approximation and including quantum tunneling effects in the framework of Feynman path integrals: KIE = k l k h = () υ l * υ h * normale [] W l 0.12em () z l 0.12em W h 0.12em () z h 0.12em k B T normale [] W l R 0.12em () z l R 0.12em W h R 0.12em () z h R 0.12em k B T where W X ( z X ) is the centroid effective potential along the reaction coordinate z X calculated from the path integrals for isotopolog X , and W X 0.12em () z X and W X R 0.25em () z X R are its values at the transition state and reactant structures. Under the harmonic approximation and neglecting quantum tunneling effects, Eq.…”
Section: The Bigeleisen Equationmentioning
confidence: 99%