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  "body": "\n## Definition\n\nLet $A$ be a unital C*-algebra and let $A \\otimes A$ denote its minimal C*-tensor product with itself.\nA *compact quantum group* is a pair $(A, \\Delta)$ where $\\Delta \\colon A \\to A \\otimes A$ is a unital $*$-homomorphism, called the comultiplication, such that:\n\n1. $(\\Delta \\otimes \\id) \\circ \\Delta = (\\id \\otimes \\Delta) \\circ \\Delta$ (coassociativity);\n2. the linear spans of $\\set{\\Delta(a)(1 \\otimes b) : a, b \\in A}$ and of $\\set{\\Delta(a)(b \\otimes 1) : a, b \\in A}$ are both norm-dense in $A \\otimes A$ (cancellation).\n\n## Remarks\n\nExample: let $G$ be a [[compact|0TVJZYB6SH]] Hausdorff group and $A = C(G)$, so that $A \\otimes A = C(G \\times G)$.\nSet $\\Delta(f)(s, t) = f(st)$.\nCoassociativity is the associativity $(rs)t = r(st)$.\nThe products $\\Delta(f)(1 \\otimes g)$ are the functions $(s, t) \\mapsto f(st) g(t)$.\nSince $(s, t) \\mapsto (st, t)$ is a homeomorphism of $G \\times G$, their span is a self-adjoint subalgebra that separates points and contains $1$.\nSo it is dense by the Stone–Weierstrass theorem, and the other span is handled in the same way.\n\nNon-example: let $S = [0, 1]$ with ordinary multiplication, a compact semigroup that is not a group, and define $\\Delta$ on $C(S)$ by the same formula.\nClause 1 holds, but every function $(s, t) \\mapsto f(st) g(t)$ is constant in $s$ on the line $t = 0$.\nThis property passes to linear combinations and uniform limits, so the span is not dense, and clause 2 fails.\n\nFor commutative $A$, every compact quantum group is of the form $C(G)$ for a compact group $G$.\nEvery compact quantum group has a unique state $h$, the Haar state, with $(h \\otimes \\id)\\Delta(a) = (\\id \\otimes h)\\Delta(a) = h(a) 1$ for all $a \\in A$; it plays the role of the Haar measure.\n",
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