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  "body": "\n## Definition\n\nLet $(M, g)$ be a closed oriented [[Riemannian manifold|7CBT4SM83Y]] of dimension $4k$.\nLet $\\Omega^*(M) = \\bigoplus_p \\Omega^p(M)$ be the space of smooth complex-valued [[differential forms|0E3G0GRPZ6]], with [[exterior derivative|0ZHSTAG8ZY]] $d$, [[Hodge star|1Y4WX4XQWJ]] $\\star$ and codifferential $\\delta$, the formal adjoint of $d$.\nDefine $\\tau \\colon \\Omega^*(M) \\to \\Omega^*(M)$ by\n$$\\tau \\omega = i^{p(p-1) + 2k} \\star \\omega \\quad \\text{for } \\omega \\in \\Omega^p(M).$$\nThen $\\tau^2 = \\id$ and $\\tau (d + \\delta) = -(d + \\delta) \\tau$.\nLet $\\Omega^\\pm(M)$ be the $\\pm 1$ eigenspaces of $\\tau$.\nThe *signature operator* of $M$ is the restriction\n$$D^+ = d + \\delta \\colon \\Omega^+(M) \\to \\Omega^-(M).$$\n\n## Remarks\n\nThe operator $d + \\delta$ is elliptic with square the [[Hodge Laplacian|PWG3GKZG80]], so $D^+$ is an [[elliptic operator|MT9P2X85V8]] of order $1$.\nIts index equals the signature $\\sigma(M)$ of the [[intersection form|WK8GKRKAVD]] on $H^{2k}(M; \\R)$.\nIndeed, the harmonic forms of degrees $p \\ne 2k$ contribute equally to the kernel and the cokernel and cancel.\nOn harmonic $2k$-forms $\\tau = \\star$, whose $\\pm 1$ eigenspaces are the self-dual and anti-self-dual forms.\nThe Atiyah–Singer index theorem applied to $D^+$ gives the [[Hirzebruch signature theorem|TEG1ZX1AGJ]].\n\nExample: on $2k$-forms, $\\tau = i^{2k(2k-1) + 2k} \\star = i^{4k^2} \\star = \\star$.\nFor $M = \\C P^2$ ($k = 1$), the harmonic $2$-forms are the multiples of the Kähler form $\\omega_{FS}$, which is self-dual, so $\\sigma(\\C P^2) = 1$ and the index of $D^+$ is $1$.\n\nNon-example: the operator $d + \\delta \\colon \\Omega^{\\mathrm{even}}(M) \\to \\Omega^{\\mathrm{odd}}(M)$ uses the splitting by degree instead of the splitting by $\\tau$.\nIt is the de Rham or Euler operator, and its index is the Euler characteristic, not the signature; for $\\C P^2$ it is $3$.\n\n## Explanations\n\n### L1 human\n\nThe signature operator is $d + d^*$ on forms, split by a twisted Hodge star, and its index is the signature of the manifold.\n",
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