More precisely, one first considers the Lie algebra spanned by generators x1, x2, x3 with Lie bracket [xi,xj] = −2εijkxk. This is well known to correspond to the simply connected Lie group S3. Then, taking the product S3×R, extending the Lie bracket so that the generator x4 is left invariant under the operation of the Lie group, and taking the quotient by αx1+βx4, where α2+β2 = 1, we finally obtain the Berger spheres B(β).
There are also higher dimensional analogues of Berger spheres.