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  "body": "\n## Definition\n\nLet $G$ be a [[locally compact group|AHV05ZBCYW]] and let $\\Gamma$ be a [[discrete subgroup|5M7D1BSHVZ]] of $G$.\nLet $G/\\Gamma$ be the space of left cosets $g\\Gamma$ with the quotient topology, on which $G$ acts by $h \\cdot g\\Gamma = hg\\Gamma$.\nThe subgroup $\\Gamma$ is a *lattice* in $G$ if there is a nonzero [[Radon measure|HZNEQQBCW4]] $\\nu$ on $G/\\Gamma$ such that:\n\n1. $\\nu$ is $G$-invariant: $\\nu(hE) = \\nu(E)$ for every $h \\in G$ and every Borel set $E \\subseteq G/\\Gamma$;\n2. $\\nu$ is finite: $\\nu(G/\\Gamma) \u003c \\infty$.\n\nA lattice $\\Gamma$ is *uniform*, or *cocompact*, if $G/\\Gamma$ is compact.\n\n## Remarks\n\nExample: $\\Z^n$ in $(\\R^n, +)$.\nThe quotient $\\R^n/\\Z^n$ is the torus, and the image of Lebesgue measure on $[0, 1)^n$ is a translation-invariant measure on it of total mass $1$.\nSince the torus is compact, $\\Z^n$ is a uniform lattice.\n\nNon-example: $\\Gamma = \\Z \\times \\set{0}$ in $\\R^2$ is discrete, but fails clause 2.\nThe quotient is the cylinder $(\\R/\\Z) \\times \\R$.\nEvery invariant Radon measure on it is a multiple of the product of the [[Haar measures|VY0HXD3GC4]] of the two factors.\nThe nonzero ones have infinite total mass.\n\nIf $G$ has a lattice, then $G$ is [[unimodular|CXG6JZGMCK]].\nA measurable [[fundamental domain|KNJA2NEZ9F]] for the action of $\\Gamma$ on $G$ by right multiplication has finite Haar measure exactly when $\\Gamma$ is a lattice.\nThe group $SL_2(\\Z)$ is a lattice in $SL_2(\\R)$ that is not uniform.\n",
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