In spherical coordinates,
$$\mathrm v (r, \theta, \phi) := \frac{1}{r^2} \hat{r} + 0 \cdot \hat{\theta} + 0 \cdot \hat{\phi} = \frac{1}{r^2} \hat{r}$$
Hence, the divergence of vector field $\mathrm v$ is given by
$$\boxed{\nabla \cdot \mathrm v = \frac{1}{r^2} \frac{\partial}{\partial r} \left( r^2 \frac{1}{r^2} \right) = 0}$$
The geometric interpretation is that the magnitude of the vector field decays inversely proportional to $r^2$, whereas the surface area of a sphere centered at the origin grows directly proportional to $r^2$. Hence, the double integral of the vector field over the surface of a sphere centered at the origin is independent of the radius $r$.
One can also use symbolic computation. In SymPy:
>>> from sympy import *
>>> x1, x2, x3 = symbols('x1 x2 x3')
>>> f1 = x1 / (sqrt(x1**2 + x2**2 + x3**2))**3
>>> f2 = x2 / (sqrt(x1**2 + x2**2 + x3**2))**3
>>> f3 = x3 / (sqrt(x1**2 + x2**2 + x3**2))**3
>>> divergence = diff(f1,x1) + diff(f2,x2) + diff(f3,x3)
>>> divergence
-3*x1**2/(x1**2 + x2**2 + x3**2)**(5/2) - 3*x2**2/(x1**2 + x2**2 + x3**2)**(5/2) - 3*x3**2/(x1**2 + x2**2 + x3**2)**(5/2) + 3/(x1**2 + x2**2 + x3**2)**(3/2)
>>> simplify(divergence)
0