Thanks, Scott Morrison
scott_re...@maths.unsw.edu.au
This is a pretty standard example in courses on Lie groups; see e.g. the
text by Graeme Segal in R. Carter, G. Segal, I. Macdonald, "Lectures on
Lie Groups and Lie Algebras", LMS Student Texts 32, Cambridge U.P.
Identify R^4 with the quaternions and SU(2) with the group of unit
quaternions. Then let SU(2)xSU(2) act on R^4 by
(q_1,q_2).v = q_1 v q_2^-1
This yields the desired morphism SU(2)xSU(2) --> SO(4).
Christian Ohn
email: christian d o t ohn a t univ h y p h e n reims a t fr
a+ib c+id
-c+id a-ib.
Then let SU(2)xSU(2) act on the 4-dimensional real vector space of
quartenions by
(U,V)Q=VQU^{-1}.
Now since determinant = norm this action is metric preserving and
therefore determines a map into SO(quartenions).
By choosing bases etc one can get explicit formulas.
Take care
Nikos.
The center of SU(2) is Z/2, generated by the scalar -1 diagonal matrix.
Therefore the center of SU(2) x SU(2) is Z/2 x Z/2, with a preferred basis
coming from the two factors.
Then SO(4) is the quotient group (SU(2) x SU(2))/ diagonal ( Z/2 \subset Z/2 x
Z/2).
--
Clarence Wilkerson \ HomePage: http://www.math.purdue.edu/~wilker
Prof. of Math. \ Internet: wil...@math.purdue.edu
Dept. of Mathematics \ Messages: (765) 494-1903, FAX 494-0548
Purdue University, \
W. Lafayette, IN 47907-1395 \
Dear Scott Morrison,
In the 1840s or 1850s (I do not know by heart) Arthur Cayley represented
points in 4D space by quaternions and found that combined left- and
right-multiplication by unit quaternions L, R amounts to a rotation about
the origin. Changing the signs of both L and R does not change the
resulting 4D rotation.
Actually, =any= 4D rotation can be represented as P -> LPR in two ways,
differing only in signs of L and R. As far as I know, Cayley failed to
prove this.
In 1897 the Dutch mathematician Lambertus van Elfrinkhof published a
formula expressing 4D rotations in terms of left and right unit quaternion
factors. He did not contend nor prove that his formula gives the =general=
4D rotation.
It is all very classical stuff. Nowadays we formulate this 150 years-old
theorem as
"S^3 x S^3 is 2:1 homomorphic to SO(4) and so as a manifold S^3 x S^3 is
the double cover of SO(4)".
Please look at http://www.xs4all.nl/~plast/So4exabs.htm for a matrix-based
proof of this theorem and for the explicit formula you want to know.
Good luck. Best regards: Johan E. Mebius