I have read in a book that the group $\mathrm{SU}(2)$ is one of the irreducible representations of the rotation group. The book begin saying that the rotation group has 3 generators $J_{1}, J_{2}$ and $J_{3}$, and the algebra is $$[J_{i},J_{j}] = i \epsilon _{ijk} J_{k}.$$ After, considering the Casimir operator $J^{2} = J_{1}^{2} + J_{2}^{2} + J_{3}^{2}$ the book finds the eigenvalues of $J^{2}$ and $J_{3}$ in the same basis: $$J^{2} |j,m \rangle = j(j + 1) |j,m \rangle ,$$ $$J_{3} |j,m \rangle = m |j,m \rangle ,$$ where $j = 0, 1/2, 1, 3/2, \ldots$ and $m = -j, -j+1,\ldots, 0, \ldots , j-1, j$. It says that for each value of $j$ corresponds one irreducible representation, for $j = 1/2$ this representation is the group $\mathrm{SU}(2)$, for $j = 1$ this is the $\mathrm{SO}(3)$, and so on...
But the book doesn't prove that this is in fact a representation. How can I do this?
And what is this rotation group? How is it defined?
Edit: I have read it in the book Matemática para físicos com aplicações by João Neto, vol. 1 (the book is in Portuguese). The book says "when two groups have the same algebra, we say that these are not two distinct groups, but different representations of the same group". So he concluded that $\mathrm{SU}(2)$ and are $\mathrm{SO}(3)$ are representations of the same group, which it call of rotation group.