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  "body": "\n## Definition\n\nA *factor* is a [[von Neumann algebra|PSFWQVZ0FS]] $M$ whose center $M \\cap M'$ is $\\C I$, where $M'$ is the [[commutant|1VC7EJ1ZBZ]].\nA *subfactor* of a factor $M$ is a von Neumann subalgebra $N \\subseteq M$ that is itself a factor and contains the identity of $M$.\nOne often writes the subfactor as the inclusion $N \\subseteq M$.\n\nIf $M$ is of type $\\mathrm{II}_1$ with faithful normal tracial state $\\tau$, let $L^2(M)$ be the Hilbert space completion of $M$ for $\\langle x, y \\rangle = \\tau(y^* x)$.\nThe *Jones index* of $N \\subseteq M$ is\n$$[M : N] = \\dim_N L^2(M) \\in [1, \\infty],$$\nthe Murray–von Neumann dimension of $L^2(M)$ as a module over $N$ acting by left multiplication.\n\n## Remarks\n\nExample: let $N$ be a $\\mathrm{II}_1$ factor and $k \\ge 1$.\nThen $N \\otimes I_k$, the matrices $\\operatorname{diag}(x, \\dots, x)$ with $x \\in N$, is a subfactor of $M = N \\otimes M_k(\\C)$, the $k \\times k$ matrices over $N$.\nBoth are factors with the same unit, and $L^2(M)$ is the direct sum of $k^2$ copies of $L^2(N)$ as an $N$-module, so $[M:N] = k^2$.\n\nNon-example: the diagonal matrices $D_2 \\subseteq M_2(\\C)$ form a unital von Neumann subalgebra of the factor $M_2(\\C)$.\nBut $D_2$ is commutative and two-dimensional, so its center is $D_2 \\ne \\C I$, and $D_2$ is not a factor.\n\nAnother example: if a finite group $G$ acts on a $\\mathrm{II}_1$ factor $M$ by outer automorphisms, the fixed-point algebra $M^G$ is a subfactor with $[M : M^G] = \\abs{G}$.\nThe index is $1$ exactly when $N = M$.\n",
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