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note
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47 refer to the assumption that the diabatic coordinates couple to the bath as the diabatic damping approximation, and their investigations suggest that it is valid over a broad set of conditions.
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The referee has pointed out that the form of eq 6 is unphysical, because it has no Taylor expansion around y = 0. Similarly, eq 7 has no Taylor expansion around y = 1/a. These forms are adopted here only to examine how different potential symmetrics affect the dynamic evolution of the excited-state packet. The true conical form of eq 5 is the one whose behavior we wish to understand; to that end, we also examine behaviors with the other forms (6-8).
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