Consider the following integral
$$J_n=\int_0^{\infty}\frac{x^{n-2}}{1+x^n}|\sin(nx)|,\:\:\:n\geq1.$$
1) Show that the above integral exists for each $n\geq 1$
2) compute $\lim_{n\to\infty}J_n$.
To show $J_n $ exists for all $n$. For a given $\epsilon$, we need to find $T\geq\frac{1}{\epsilon}$, such that
$$\int_T^{\infty}\frac{x^{n-2}}{1+x^n}|\sin(nx)|\leq \epsilon.$$
Now let $T\geq\frac{1}{\epsilon}.$ Hence $$\big{|}\int_0^{\infty}\frac{x^{n-2}}{1+x^n}|\sin(nx)|dx-\int_0^T\frac{x^{n-2}}{1+x^n}|\sin(nx)|dx\big{|}\leq\int_T^{\infty}\big{|}\frac{x^{n-2}}{1+x^n}|\sin(nx)|dx\leq\int_T^{\infty}\frac{1}{x^2}dx=\lim_{M\to\infty}{\frac{-1}{M}}+\frac{1}{T}\leq\epsilon.$$
Now for the second part I'm thinking about using the Riemann Lebesgue lemma.
Note that $\lim_{n\to\infty}\frac{x^{n-2}}{1+x^n}=0$, when $x\in[0,1)$, and $\lim_{n\to\infty}\frac{x^{n-2}}{1+x^n}=\frac{1}{x^2}$, when $x\in[1,\infty).$
Now, by extended Riemann Lebesgue lemma, we have $\lim_{n\to\infty}\int_0^{\infty}\frac{1}{x^2}|\sin(nx)|dx=\frac{2}{\pi}. $
So I'm gussing the limit must be $\frac{2}{\pi}$. However I don't know hwo to make a vigorous argument. Also, I'm not sure about the first part. Thank you.
1. For the first part, when $x \geq 1$ we have
$$ \frac{x^{n-2}}{1+x^n}|\sin(nx)| \leq \frac{x^{n-2}}{1+x^n} \leq \frac{1}{x^2}$$
and if $0\leq x \leq 1$ we have
$$ \frac{x^{n-2}}{1+x^n}|\sin(nx)| \leq x^{n-2}|\sin(nx)| \leq 1. $$
(Indeed, when $n \geq 2$, the last inequality its trivial by bounding $x^{n-2} \leq 1$ and $|\sin(nx)|\leq 1$. When $n = 1$, we can utilize the bound $|\sin x| \leq |x|$ to obtain $x^{n-2}|\sin x| = x^{-1}|\sin x| \leq 1$.)
So the integrand is bounded by the integrable function $1 \wedge x^{-2}$ and hence the integral exists.
2. For the second part, let me prove the following general proposition.
Before proving this proposition, let us first enjoy its consequence. Since we know that $x \mapsto \frac{x^{n-2}}{1+x^n}$ is bounded by $1\wedge x^{-2}$ for $n \geq 2$ and converges to $x^{-2} \mathbf{1}_{(1,\infty)}(x)$ a.e., by (2) we have
$$ \lim_{n\to\infty} J_n = \frac{2}{\pi} \int_{1}^{\infty} x^{-2} \, dx = \frac{2}{\pi}. $$
Proof of Proposition. (1) First consider the case where $f \in C_c(\mathbb{R})$ is continuous and compactly supported. Then
\begin{align*} \int_{\mathbb{R}} f(x)|\sin(nx)| \, dx &= \frac{1}{n}\int_{\mathbb{R}} f(x/n)|\sin(x)| \, dx \\ &= \frac{1}{n}\sum_{k\in\mathbb{Z}}\int_{0}^{\pi} f\left(\frac{x+k\pi}{n}\right)\sin(x) \, dx \\ &= \int_{0}^{\pi} \left( \frac{1}{n}\sum_{k\in\mathbb{Z}}f\left(\frac{x}{n}+\frac{k\pi}{n}\right) \right) \sin(x) \, dx \end{align*}
Here, the sum and the integral can be interchanged freely because for each fixed $n$ there are only finitely many non-zero terms. Also, using the assumption on $f$ it is not hard to show that
$$ \frac{1}{n}\sum_{k\in\mathbb{Z}}f\left(\frac{x}{n}+\frac{k\pi}{n}\right) \xrightarrow[n\to\infty]{} \frac{1}{\pi}\int_{\mathbb{R}} f(t) \, dt $$
uniformly in $x$. So it follows that
$$ \int_{\mathbb{R}} f(x)|\sin(nx)| \, dx \xrightarrow[n\to\infty]{} \frac{1}{\pi} \left( \int_{\mathbb{R}} f(x) \, dx \right)\left( \int_{0}^{\pi} \sin x \, dx \right) = \frac{2}{\pi} \int_{\mathbb{R}} f(x) \, dx. $$
For general integrable $f$, the usual approximation argument works perfectly: Let $\varphi \in C_c(\mathbb{R})$ be any continuous and compactly supported function and notice taht
\begin{align*} &\left| \int_{\mathbb{R}} f(x)|\sin(nx)| \, dx - \frac{2}{\pi} \int_{\mathbb{R}} f(x) \, dx \right|\\ &\hspace{2em} \leq \left| \int_{\mathbb{R}} f(x)|\sin(nx)| \, dx - \int_{\mathbb{R}} \varphi(x)|\sin(nx)| \, dx \right| \\ &\hspace{3em} + \left| \int_{\mathbb{R}} \varphi(x)|\sin(nx)| \, dx - \frac{2}{\pi} \int_{\mathbb{R}} \varphi(x) \, dx \right| \\ &\hspace{3em} + \left| \frac{2}{\pi} \int_{\mathbb{R}} \varphi(x) \, dx - \frac{2}{\pi} \int_{\mathbb{R}} f(x) \, dx \right| \\ &\hspace{2em} \leq \left(1 + \frac{2}{\pi}\right) \| f - \varphi\|_{L^1} + o(1). \end{align*}
So it follows that
$$ \limsup_{n\to\infty} \left| \int_{\mathbb{R}} f(x)|\sin(nx)| \, dx - \frac{2}{\pi} \int_{\mathbb{R}} f(x) \, dx \right| \leq \left(1 + \frac{2}{\pi}\right) \| f - \varphi\|_{L^1}. $$
But since the LHS is a constant independent of $\varphi$ and $C_c(\mathbb{R})$ is dense in $L^1(\mathbb{R})$, we may let $\varphi \to f$ to show that the LHS is $0$. Therefore (1) follows.
(2) We have
\begin{align*} &\left| \int_{\mathbb{R}} f_n(x)|\sin(nx)| \, dx - \frac{2}{\pi} \int_{\mathbb{R}} f(x) \, dx \right|\\ &\hspace{2em} \leq \left| \int_{\mathbb{R}} f_n(x)|\sin(nx)| \, dx - \int_{\mathbb{R}} f(x)|\sin(nx)| \, dx \right| \\ &\hspace{3em} + \left| \int_{\mathbb{R}} f(x)|\sin(nx)| \, dx - \frac{2}{\pi} \int_{\mathbb{R}} f(x) \, dx \right| \\ &\hspace{2em} \leq \| f_n - f \|_{L^1} + o(1). \end{align*}
By the dominated convergence theorem, we know that $f_n \to f$ in $L^1$. Therefore (2) follows from the previous part.