Re: Lie group F4 = Aut(OP2)
- From: baez@xxxxxxxxxxxxxx (John Baez)
- Date: Tue, 14 Feb 2006 14:28:03 +0000 (UTC)
In article <7595736.1139632166640.JavaMail.jakarta@xxxxxxxxxxxxxxxxxxxxxx>,
Marek Mitros <marekmit@xxxxxxxxxxxx> wrote:
Some poor uncited soul wrote:
Indeed (non-)associativity spoils the conventional
technique of using
equivalence classes of scale invariant coordinates to
construct OP^3
Instead one defines OP^3 using the exceptional Jordan
algebra J(3,O),
where points of OP^3 consist of those matrices of
J(3,O) with vanishing
Freudenthal product (A x A = 0).
You mean to say "nonzero matrices in J(3,O) with A x A = 0, modulo
multiplication by nonzero real numbers".
Thank you for this answer. However it is not enough for me. This
definition is not intuitive enough, not geometrical enough for me. I
would like to imagine how the OP2 looks.
I urge you to read this:
http://math.ucr.edu/home/baez/octonions/node8.html
I start from very geometrical considerations and sketch how
points in projective spaces wind up being described as rank-1
projections in formally real Jordan algebras.
Then here:
http://math.ucr.edu/home/baez/octonions/node12.html
I describe points in the octonionic projective plane OP^2 as
rank-1 projections in the exceptional Jordan algebra.
Then, I explain the Freudenthal cross product x in the exceptional
Jordan algebra.
Then, I report Freudenthal's observation that the rank-1
projections in the exceptional Jordan algebra are the same
as nonzero elements with A x A = 0, modulo multiplication
by nonzero real numbers.
You will have to do some calculations to verify this claim,
and/or look at Freudenthal's paper.
But, if you're trying to work with points and lines in
OP^2, the Freudenthal cross product is very useful.
Do you know any analogy of the Jordan algebra and OP2 to quaternions?
The self-adjoint 3x3 real, complex or quaternionic matrices also form
a Jordan algebra, and the rank-1 projections in here are the points
in the real, complex and quaternionic projective plane, respectively.
But an even simpler example is CP^1, and that's a good place to
start:
http://math.ucr.edu/home/baez/octonions/node11.html
since it's the heavenly sphere!
.
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