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These types of KIEs have classically been explained in terms of a difference between C-H/D bond distances (a consequence of the anharmonicity of the potential function and the different ZPEs of the C-H/D bonds) and this is the context in which we frame our introduction. As we subsequently describe, these IEs are more fully explained by changes in the shape of potential energy wells at the transition state and the differences in coupling of vibrational modes with the host deformation.
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