It is given that X has a pdf of
$f_X(x)$ = $\frac{sin(\pi r)}{\pi x}$$(x - \theta)^{-r}$$\theta^r$ for $x>\theta$, and
$f_X(x)$ = $0$ for $0 Question: Show that $f_X(x)$ is a pdf. I am familiar with the properties that define a pdf, and however I am confused with how to go about showing the part of the definition that states: $\int f_X(x)$ $dx=1$ My attempt: $\int \frac{sin(\pi r)}{\pi x}$$(x - \theta)^{-r}$$\theta^r$ $dx$ = $\frac{sin(\pi r)}{\pi}$ $\int $$(x - \theta)^{-r}$$\theta^r$$x^{-1}$ $dx$ = $\frac{sin(\pi r)}{\pi}$ $\int \left(\frac{\theta}{x - \theta}\right)^r$$x^{-1}$ $dx$ This is the part where I keep getting confused. I know that I need to use the Gamma function identity: $\Gamma(a)\Gamma(1-a)$ = $\frac{\pi}{sin(\pi a)}$. As well as, an integral representation of the Beta function: $B(a,b)=\frac{\Gamma(a)\Gamma(b)}{\Gamma(a+b)}$ (which I'm torn between $B(a,b)=\int_0^1 t^{a-1}(1-t)^{b-1} dt$ or $B(a,b)=\int_0^\infty \frac{t^{a-1}}{(t+1)^{a+b}} dt$) I'd really appreciate some guidance on how to apply the representation of the Beta function to the function within the integral.