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  "body": "\n## Definition\n\nLet $H$ be a complex [[Hilbert space|HM2HHE3J51]] and let $B(H)$ be the [[algebra of bounded operators|BMDG4JQPEH]] on $H$.\nLet $A$ be a unital $*$-subalgebra of $B(H)$.\nLet $D$ be a densely defined [[unbounded|KRJX5RA0PW]] [[self-adjoint operator|0NEGN5CRSC]] on $H$ with domain $\\operatorname{dom} D$.\nThe triple $(A, H, D)$ is a *spectral triple* if:\n\n1. for every $a \\in A$, the operator $a$ maps $\\operatorname{dom} D$ into itself, and the commutator $[D, a] = Da - aD$ on $\\operatorname{dom} D$ extends to a bounded operator on $H$;\n2. the resolvent $(D - \\lambda I)^{-1}$ is a [[compact operator|M2NEP1K5AE]] for one, and then for every, $\\lambda \\in \\C \\setminus \\R$.\n\n## Remarks\n\nExample: let $A = C^\\infty(S^1)$ act on $H = L^2(S^1)$ by multiplication and let $D = -i \\, d/d\\theta$ on the Sobolev space of functions with square-integrable derivative.\nThe functions $e_n(\\theta) = e^{in\\theta}$, $n \\in \\Z$, form an orthonormal basis of eigenvectors with $D e_n = n e_n$, so $(D - i)^{-1}$ has eigenvalues $1/(n - i) \\to 0$ and is compact.\nFor $f \\in A$ the product rule gives $[D, f] = -i f'$, which is multiplication by a bounded function.\nMore generally, smooth functions on a compact Riemannian spin manifold, acting on square-integrable spinors, with the [[Dirac operator|3DXGJTEQZH]], form a spectral triple.\n\nNon-example: if $H$ is infinite-dimensional and $D = 0$, every commutator is $0$, so clause 1 holds.\nBut $(D - i I)^{-1} = i I$ is not compact, so clause 2 fails.\n\nOften $A$ is a dense $*$-subalgebra of a C*-algebra, and $A$ acts on $H$ through a faithful $*$-representation.\nA spectral triple is called even if there is a self-adjoint unitary $\\gamma$ on $H$ that commutes with $A$ and anticommutes with $D$.\nFor two states $\\varphi$ and $\\psi$ of the norm closure of $A$, Connes' distance formula is\n$$d(\\varphi, \\psi) = \\sup \\set{ \\abs{\\varphi(a) - \\psi(a)} : a \\in A, \\ \\|[D, a]\\| \\le 1 }.$$\nIt recovers the geodesic distance when $\\varphi$ and $\\psi$ are evaluations at two points of a manifold.\n",
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