The potential slow-roll parameter is
From the slow-roll approximation,
Therefore
Thus implies , consistently with potential-energy domination.
The same equations give
On the branch , the definition of turns this into
By definition,
Using and the result of part (a),
Reversing the limits yields the slow-roll e-fold count
For the natural inflation potential, write . Then
and the half-angle identity gives
Therefore, on the stated rolling branch,
Substitution into part (b) gives
Since
the e-fold count for the natural-inflation cosine potential is

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