Can anyone give me an explicit isomorphism between $SU(2)$ and the three sphere?
What about for higher spheres? This question link text seems to indicate that there exists a homeomorphism from $SU(n)/SU(n1)$ to the $(2n1)$sphere.
Can anyone give me an explicit isomorphism between $SU(2)$ and the three sphere? What about for higher spheres? This question link text seems to indicate that there exists a homeomorphism from $SU(n)/SU(n1)$ to the $(2n1)$sphere. 


Elements of $SU(2)$ look like this: $$ x = \begin{pmatrix} a &  \overline{b} \\ b & \overline{a} \end{pmatrix},$$ where $a^2 + b^2 = 1$. This follows easily from $x^* = x^{1}$. So you map that matrix to the point $(a,b)$ in $\mathbb{C}^2$, and this is your diffeomorphism. 


$SU(2)$ is a group of unitary quaternions $U(1,H)$, which are of form $a + bI + cJ + dK$, with $a^2+b^2+c^2+d^2=1$. This is clearly $S^3$. The action of unitary quaternions from the right preserves complex structure acting from the left (or vice versa), this gives a map from $U(1,H)$ to $U(2)$. It also preserves the complex volume, because quaternionic structure can be used to define the symplectic form. 


Regarding the higher dimensional question: Please try to figure this out yourself. Just think about the map from SU(n) to $C^n$, mapping each matrix to the first column. What is the image and what is the preimage of each point in the image? Hint: confirm that it suffices to figure out the preimage of (1,0,...,0) and all other preimages are essentially the same. 


Just write $SU(2)$ in some local coordinates (some of the standard systems are the doublepolar system (a.k.a Hyperspherical coordinates) or the single angle coordinates (a.k.a Hopf coordinates) and then one sees that the special unitary condition forces the $4$ parameters you will need to satisfy the $3$sphere equation. Hence one gets an explicit local map to the $3$sphere by mapping that matrix to the ordered tuple of $4$ numbers. Smoothness is assured since the functions are all polynomials. These coordinate systems make what MTS said below explicit. After all one is very likely to want to do some geometry on $SU(2)$ now that one knows it is $S^3$ and these coordinate systems are naturally adapted to do them. Like computing vielbiens on $SU(2)$ in these systems look very natural and make the symmetries of the spherical structure underneath very clear. A related extra stuff: One can look up a very nice analysis of this in the first chapter of Gregory Naber's book "Geometry, Topology and Gauge Fields" Volume 1. In that section he will do what gets called the Heegard Decomposition of $S^3$ using very simple highschool maths! Basically Naber will rationalize why these coordinate systems are in some sense natural. You can also look up these analysis in these two writeups I had done during my undergrad , this and this one. 

