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  "body": "\n## Proof\n\nDefine the following operator on compactly supported functions on $\\Gamma\\backslash G$:\n\n$$R(\\phi) = \\int_G \\phi(x)R(x)\\,dx.$$\n\nIt extends continuously to $L^2(\\Gamma\\setminus G)$ and for $f\\in L^2(\\Gamma\\setminus G)$ we have:\n\n$$(R(\\phi)f)(x) = \\int_G\\phi(y)f(xy)\\,dy = \\int_{\\Gamma\\setminus G}\\left(\\sum_{\\gamma\\in\\Gamma}\\phi(x^{-1}\\gamma y)\\right)f(y)\\,dy$$\n\nafter a change of variables. Assuming $\\Gamma\\setminus G$ is compact, the operator $R(\\phi)$ is trace-class and the trace formula is the result of computing its trace in two ways as explained below.\n\nThe trace of $R(\\phi)$can be expressed as the integral of the kernel $K(x,y)=\\sum_{\\gamma\\in\\Gamma}\\phi(x^{-1}\\gamma y)$ along the diagonal, that is:\n\n$$\\operatorname{tr}R(\\phi) = \\int_{\\Gamma\\setminus G}\\sum_{\\gamma\\in\\Gamma}\\phi(x^{-1}\\gamma x)\\,dx.$$\n\nLet $\\{\\Gamma\\}$ denote a collection of representatives of conjugacy classes in $\\Gamma$, and $\\Gamma^\\gamma$ and $G^\\gamma$ the respective centralizers of $\\gamma$. Then the above integral can, after manipulation, be written\n\n$$\\operatorname{tr}R(\\phi) = \\sum_{\\gamma\\in\\{\\Gamma\\}} a_\\Gamma^G(\\gamma)\\int_{G^\\gamma\\setminus G}\\phi(x^{-1}\\gamma x)\\,dx.$$\n\nThis gives the *geometric side* of the trace formula.\n\nThe *spectral side* of the trace formula comes from computing the trace of $R(\\phi)$ using the decomposition of the regular representation of $G$ into its irreducible components. Thus\n\n$$\\operatorname{tr}R(\\phi) = \\sum_{\\pi\\in\\hat G}a_\\Gamma^G(\\pi)\\operatorname{tr}\\pi(\\phi)$$\n\nwhere $\\hat G$ is the set of irreducible unitary representations of $G$ (recall that the positive integer $a_\\Gamma^G(\\pi)$ is the multiplicity of $\\pi$ in the unitary representation $R$ on $L^2(\\Gamma\\setminus G)$).\n",
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        "locator": "Selberg trace formula, section The general Selberg trace formula for cocompact quotients \u003e Proof",
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