Notice that the matrix $$P=\frac{11^T}{n}$$ is an orthoprojector, meaning $P^2=P=P^T$.
Such matrices are also called idempotent, and they have just 2 distinct eigenvalues $\{0,1\},\,$ since those are the only 2 idempotent scalars.
You wish to evaluate the function
$$f(x)=(n+nx)^{-1}$$
with a matrix argument of $P$, i.e.
$$f(P)=(nI+nP)^{-1}$$
Now the nice thing about an idempotent matrix is that the power series for any function only has 2 terms
$$f(P) = c_0I+c_1P$$ Using Sylvester Interpolation, substitute each eigenvalue into the function and into the power series
$$\eqalign{
f(1) &= \frac{1}{2n} &= c_0+c_1 \cr
f(0) &= \frac{1}{n} &= c_0 \cr
}$$ and solve for the coefficients.
Looks like $c_0$ is already "solved", and the remaining coefficient is simply
$$c_1 = \frac{1}{2n}-\frac{1}{n} =-\frac{1}{2n}$$
Therefore
$$\eqalign{
f(P) &= \frac{1}{n}I-\frac{1}{2n}P \cr
&= \frac{1}{n}\Big(I-\frac{1}{2}P\Big) \cr
&= \frac{1}{n}\Big(I-\frac{1}{2n}11^T\Big) \cr\cr
}$$
Update
Since you can't find anything on Sylvester interpolation, let me work out a second example.
Let's say that you wanted to calculate the exponential rather than the inverse of your matrix.
$$\exp(nI+11^T)=\exp(nI+nP)$$
This corresponds to the scalar function
$$f(x)=\exp(n+nx)$$
We have the same 2-term series expansion as last time
$$f(P)=c_0I+c_1P$$
Substituting the eigenvalues yields
$$\eqalign{
f(1) &= e^{n+1} &= c_0+c_1 \cr
f(0) &= e^n &= c_0 \cr
}$$
Once again, the $c_0$ is "solved" and the remaining coefficient is
$$c_1=e^{n+1}-e^{n}=e^{n}(e-1)$$
Therefore we have
$$\eqalign{
\exp(nI+11^T)
&= e^{n}I+e^{n}(e-1)P \cr
&= e^{n}\Big(I+\frac{e-1}{n}11^T\Big) \cr
}$$