Jordan algebra and quaternionic projective space How we can define quaternionic projective space and metric on it using Jordan algebra?
Thank you in advance!
 A: I am not much educated in this subject so please take my answer with a grain of salt. 
The appropriate Jordan algebra is $J_n(\mathbb{H}) := \{ A \in M(n,\mathbb{H})\\,|\\, \overline{A}^T=A \}$ with multiplication defined as $A\circ B = (AB+BA)/{2}$. The metric is defined by $\mathrm{Tr}(A^2)$. The quaternionic projective space can be then defined as the space of elements of $J_n(\mathbb{H})$ of rank one and trace one (think of these matrices as projectors to one-dimensional subspaces) or alternatively as the (real) projectivization of rank one matrices. 
I am little bit more familiar with the case of octonionic projective plane, so let me explain that case. There the relevant algebra is $J_3(\mathbb{O})$ and the plane $\mathbb{OP}^2$ and its metric is defined in the same way[1] as in the quaternionic case. Now there is a well defined cubic form on $J_3(\mathbb{O})$ which is basically the determinant. The group that preserves this cubic form is $E_6$. In fact one defines some sort of cross product (I think it is called Jordan cross product.) out of the cubic form which then gives the incidence relation of the projective geometry of $\mathbb{OP}^2$. If I remember correctly, the   product $A\times B$ is defined by the relation $(A\times B,C) = (A,B,C)$, where on the left hand side the brackets denote the polarization of the quadratic form while on the right hand side the brackets denote the polarization of the cubic form. The group $E_6$ is then the  group of collineations of $\mathbb{OP}^2$
The group that preserves the determinant and the quadratic form (the norm) is the group $F_4$. This sheds some light on the fact that $F_4$ is in fact the isometry group of $\mathbb{OP}^2$. It can be proven that $F_4$ is in fact the automorphism group of the Jordan algebra $J_3(\mathbb{O})$!
In the quaternionic case one finds that $E_6$ is replaced by $Sl(n,\mathbb{H})$ and $F_4$ by $Sp(n)$.
The projective plane $\mathbb{OP}^2$ was much studied by Freudenthal and others but I do not know of any reference where the quaternionic case is treated via Jordan algebras.
[1] Of course one needs to be a little careful with the definition of rank because of the nonassociativity of $\mathbb{O}$. Either one uses the fact that any element of $J_3(\mathbb{O})$ can be mapped by the action of $F_4$ to a diagonal matrix and then one defines the rank by the number of nonzero elements in this diagonalization. Or one can experiment a little bit and discover that it is possible to define determinants of 2x2 minors in such a way that their vanishing is equivalent to matrix of being of rank one according to first definition. 
A: (Perhaps my answer will be too general for your purposes.)
The description of the projective space that you mention, is only one special case of a very general construction (due to O. Loos) of a projective space from a Jordan pair, which is a pair of vector spaces $(V^+, V^-)$ equipped with certain quadratic operators. The notion of a Jordan pair generalizes the notion of a Jordan algebra, in the sense that any Jordan algebra $J$ can be made into a Jordan pair (but the converse is not true).
If $V = (V^+, V^-)$ is such a Jordan pair, then the projective space $X(V)$ of $V$ is the quotient of $V^+ \times V^-$ by projective equivalence, defined as
$$ (x, y) \sim (x', y') \iff (x, y - y') \text{ is quasi-invertible, and } x' = x^{y-y'}, $$
where $x^{y-y'}$ denotes the quasi-inverse of the pair $(x, y-y')$.
In the case where $V$ is the Jordan pair arising from the Jordan algebra of hermitian matrices over any skew field $D$ (of which $D = \mathbb{H}$ is just a particular case), the projective space $X(V)$ is the classical projective space coordinatized by the skew field $D$.
