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. Author manuscript; available in PMC: 2013 Aug 28.
Published in final edited form as: Biochemistry. 2012 Aug 15;51(34):6860–6870. doi: 10.1021/bi300613e

Figure 7.

Figure 7

Comparison of the wavefunction overlap between donor (blue) and acceptor (red) states of 1H for the nonadiabatic limit, using Morse potentials (top), and the adiabatic limit used in the present calculations (bottom). In both examples the DAD is set at 3.2 Å. The Morse wavefunctions are the ground eigenstates of the Hamiltonian and the wavefunctions for the double-well potential were constructed as linear combinations of the ground and first excited eigenstates of the Hamiltonian.