What is known about f(k)=∑k−1n=0knn! for large k?
Obviously it is is a partial sum of the series for ek -- but this partial sum doesn't reach close to ek itself because we're cutting off the series right at the largest terms. In the full series, the (k+i−1)th term is always at least as large as the (k−i)th term for 1≤i≤k, so f(k)<ek/2. Can we estimate more precisely how much smaller than ek the function is?
It would look very nice and pleasing if, say, f(k)∼ek−1 for large k, but I have no real evidence for that hypothesis.
(Inspired by this question and my answer thereto).
Answer
This appears as problem #96 in Donald J Newman's excellent book: A Problem Seminar.
The problem statement there is:
Show that
1+n1!+n22!+⋯+nnn!∼en2
Where an∼bn mean lim.
Thus we can estimate your sum (I have swapped n and k) as
1 + \frac{n}{1!} + \frac{n^2}{2!} + \dots + \frac{n^{n-1}}{(n-1)!} \sim \frac{e^n}{2}
as by Stirling's formula, \dfrac{n^n}{n!e^n} \to 0.
The solution in the book proceeds as follows:
The remainder term for a the Taylor Series of a function f is
R_n(x) = \int_{0}^{x} \frac{(x-t)^n}{n!} f^{n+1}(t) \ \text{d}t
which for our purposes, comes out as
\int_{0}^{n} \frac{(n-t)^n}{n!} e^t \ \text{d}t
Making the substitution n-t = x gives us the integral
\int_{0}^{n} \frac{x^n}{n!} e^{-x} \ \text{d}x
In an earlier problem (#94), he shows that
\int_{0}^{\infty} \left(1 + \frac{x}{n}\right)^n e^{-x} \ \text{d}x \sim \sqrt{\frac{\pi n}{2}}
which using the substitution n+x = t gives
\int_{n}^{\infty} t^n e^{-t} \ \text{d}t \sim \frac{n^n}{e^n} \sqrt{\frac{\pi n}{2}}
Using \int_{0}^{\infty} x^n e^{-x}\ \text{d}x = n! and Stirling's formula now gives the result.
To prove that
\int_{0}^{\infty} \left(1 + \frac{x}{n}\right)^n e^{-x} \ \text{d}x \sim \sqrt{\frac{\pi n}{2}}
He first makes the substitution x = \sqrt{n} t to obtain
\int_{0}^{\infty} \left(1 + \frac{x}{n}\right)^n e^{-x} \ \text{d}x \ = \sqrt{n} \int_{0}^{\infty} \left(1 + \frac{t}{\sqrt{n}}\right)^n e^{-\sqrt{n} t} \ \text{d}t
Now \left(1 + \frac{t}{\sqrt{n}}\right)^n e^{-\sqrt{n} t} \le (1+t)e^{-t} and thus by the dominated convergence theorem,
\lim_{n\to \infty} \frac{1}{\sqrt{n}} \int_{0}^{\infty} \left(1 + \frac{x}{n}\right)^n e^{-x} \ \text{d}x
= \int_{0}^{\infty} \left(\lim_{n \to \infty}\left(1 + \frac{t}{\sqrt{n}}\right)^n e^{-\sqrt{n} t}\right) \ \text{d}t
= \int_{0}^{\infty} e^{-t^2/2} \ \text{d}t = \sqrt{\frac{\pi}{2}}
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