Let $X$ be a non-negative discrete random variable such that $0\le X\le B$ and$$f(n)=\frac{E^2[X^n]}{E[X^{n-1}]E[X^{n+1}]}$$for $n \ge 1$.
I am interested in the rate of growth of $f(n)$ as $n \to \infty$. In other words, is there a way to quantify how fast $f(n)$ approaches its limit as a function of $n$ and some “property” of $X$?
A few observations:
- Upper bound: By Cauchy-Schwarz we have that $f(n) \le 1$.
- Exact limit: It can be shown that $\lim\limits_{n \to \infty} f(n)=1$. So, we are trying to refine this limit.
- Trivial example: If $X$ is supported on $\{0,B\}$, then $f(n)= 1$ for all $n \ge 1$.
- Connection to Strong Cauchy-Schwarz: Essentially, this is a question about the sharper versions of Cauchy-Schwartz inequality. Therefore, using the expression for the correction term in Cauchy-Schwartz we have $$ f(n)=1-\frac{1}{2} E \left[ \left| \frac{X^\frac{n-1}{2}}{ \sqrt{E[X^{n-1}]}} -\frac{X^\frac{n+1}{2}}{ \sqrt{E[X^{n+1}]}}\right|^2 \right]. $$
I would like to answer this with minimal assumptions, but, if needed, we can assume there is a mass at $B$.
Try checking out Problem 7.2 in Steele's The Cauchy-Schwarz Master Class. I'll write the statement of this problem:
Yes, this problem technically deals with continuous distributions and assumes a nonincreasing density function $f$. But looking through the proof in the book, I fail to see why we need $f$ to be nonincreasing; it seems that $\int_0^\infty x^{2\max(\alpha, \beta)} f(x) dx < \infty$ is enough from my reading of Steele's proof. Assuming that this problem passes onto the discrete case, we can let $\alpha = \frac{1}{2}(n-1), \beta = \frac{1}{2}(n+1)$ to achieve \begin{align*} \frac{E^2[X^n]}{ E[X^{n-1}] E[X^{n+1}]} \le 1 - \frac{1}{(n+1)^2} \end{align*} Therefore, the ratio approaches 1 at a rate that is at least (EDIT: thanks to River Li, it should be "at most") quadratic in $n$.