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  "body": "\n## Definition\n\nLet $F$ be a [[field|0QA8CHH8MG]] of characteristic different from $2$.\nA *Jordan algebra* over $F$ is a [[vector space|05EGHEQZAW]] $J$ over $F$ with a bilinear product $J \\times J \\to J$, $(x, y) \\mapsto xy$, such that for all $x, y \\in J$:\n\n1. $xy = yx$;\n2. $(xy)(xx) = x(y(xx))$.\n\nClause 2 is the *Jordan identity*.\nThe product need not be associative, so $J$ is a [[nonassociative ring|YP5TQ6WFVN]] with an $F$-vector space structure.\n\n## Remarks\n\nExample: for an associative $F$-algebra $A$, put $x \\circ y = \\frac{1}{2}(xy + yx)$.\nClause 1 is clear, and clause 2 follows by expanding: with $x^2 = xx$ in $A$, one has $x \\circ x = x^2$, and both $(x \\circ y) \\circ x^2$ and $x \\circ (y \\circ x^2)$ equal $\\frac{1}{4}(xyx^2 + yx^3 + x^3y + x^2yx)$.\nThe resulting Jordan algebra is written $A^+$; the Hermitian $n \\times n$ complex matrices form a real Jordan subalgebra of $M_n(\\C)^+$.\nNon-example: $\\R^3$ with the cross product satisfies clause 2, since $x \\times x = 0$ makes both sides $0$, but fails clause 1, because $x \\times y = -y \\times x$.\nA Jordan algebra is power-associative: the powers of a single element do not depend on the bracketing.\n",
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