Integrals over a space with Lorentz signature metric

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$$\int_{spacetime}\frac{d^4x}{(x^2)^2}=\int_{-\infty}^{\infty} dt\int_{-\infty}^{\infty} dx\int_{-\infty}^{\infty} dy\int_{-\infty}^{\infty} dz\frac{1}{(t^2-x^2-y^2-z^2)^2}$$ To show that $\int_{spacetime}\frac{d^4x}{(x^2)^2}$ diverges in physics we use this type of non rigourous arguments $$d^4x\approx k|x|^3d|x|\implies \int_{spacetime}\frac{d^4x}{(x^2)^2}=\int_{0}^{\infty}\frac{k|x|^3d|x|}{|x|^4}=\int_{0}^{\infty}{kd(ln|x|)}=\text{diverges}$$

Can someone rigorously prove the above relation? Example here they did like that.

The main problem is $x^2$ can be $<0$ so $|x|$ can be imaginary. So the above method is not straightforward without proper justification.

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You can always use Tonelli's theorem and then go to the usual 3D polar coordinates. SO, the integral $I$ can be calculated as \begin{align} I&=\int_{\Bbb{R}^3}\int_{\Bbb{R}}\frac{1}{(t^2-x^2-y^2-z^2)^2}\,dt\, d(x,y,z)\tag{Fubini-Tonelli}\\ &=\int_{0}^{\infty}\int_{\Bbb{R}}\frac{1}{(t^2-r^2)^2}\,dt\cdot 4\pi r^2\,dr\tag{Polar coordinates}\\ &=8\pi\int_0^{\infty}\int_0^{\infty}\frac{r^2}{(t^2-r^2)^2}\,dt\,dr\tag{evenness} \end{align} Now, for each $r\in (0,\infty)$, we have $\int_0^{\infty}\frac{r^2}{(t^2-r^2)^2}\,dt=r^2\int_0^{\infty}\frac{1}{(t-r)^2(t+r)^2}\,dt=\infty$, because the singularity at $t=r$ is a quadratic $\frac{1}{(t-r)^2}$, and these are not integrable singularities (look up the integral p-tests from single variable calculus). Since for each $r\in (0,\infty)$ the inner integral is $\infty$, the whole thing is $\infty$: \begin{align} I&=8\pi\int_0^{\infty}\infty\,dr=\infty. \end{align}