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  "body": "\n## Definition\n\nLet $\\mathbb{H}$ be the [[upper half-plane|X6XGGH5FPW]], let $E_4$ and $E_6$ be the normalized [[Eisenstein series|EYREVY31BN]] of weights $4$ and $6$, and let $\\Delta = (E_4^3 - E_6^2)/1728$.\nThe *$j$-invariant* is the function $j \\colon \\mathbb{H} \\to \\C$ given by\n$$j(\\tau) = \\frac{E_4(\\tau)^3}{\\Delta(\\tau)} = \\frac{1728\\, E_4(\\tau)^3}{E_4(\\tau)^3 - E_6(\\tau)^2}.$$\n\n## Remarks\n\nThe [[cusp form|A50Y012RBP]] $\\Delta$ has no zeros on $\\mathbb{H}$, so $j$ is holomorphic on $\\mathbb{H}$.\nBoth $E_4^3$ and $\\Delta$ have weight $12$, so $j(\\gamma \\tau) = j(\\tau)$ for every $\\gamma$ in the [[modular group|VEKV1EM77B]].\nWith $q = e^{2 \\pi i \\tau}$, $j(\\tau) = q^{-1} + 744 + 196884 q + \\cdots$, so $j$ is a [[meromorphic|0ZZ7ZYDR8W]] modular function with a simple pole at infinity.\nExample: $E_6(i) = 0$, so $j(i) = 1728$; and $E_4(e^{2 \\pi i/3}) = 0$, so $j(e^{2 \\pi i /3}) = 0$.\nNon-example: $j$ is not a [[modular form|GWKN5VG78A]] of weight $0$, because it is unbounded as $\\operatorname{Im} \\tau \\to \\infty$.\nFor the elliptic curve $y^2 = x^3 + ax + b$, the $j$-invariant is $1728 \\cdot 4a^3 / (4a^3 + 27b^2)$.\n",
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