Wednesday, May 29, 2019

real analysis - Partial sums of exponential series



What is known about f(k)=k1n=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+i1)th term is always at least as large as the (ki)th term for 1ik, 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)ek1 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 anbn 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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