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  "body": "\n## Summary\n\nA modular form of weight $k$ is a [[holomorphic function|0NAHXR1FRH]] on the [[upper half-plane|X6XGGH5FPW]].\nIt transforms in a fixed way under the [[modular group|VEKV1EM77B]] and stays bounded at infinity.\nIts Fourier expansion $\\sum_{n \\ge 0} a_n q^n$ in $q = e^{2 \\pi i \\tau}$ often has arithmetic coefficients.\nThe spaces of modular forms of a given weight are finite-dimensional, so identities between them can be proved by comparing a few coefficients.\nModular forms are central in modern number theory, for example in the proof of Fermat's Last Theorem through the [[modularity theorem|CS1NVJBZMH]].\n\n## Explanations\n\n### L1 human\n\nA modular form is a function with an enormous amount of symmetry.\nIt is periodic, $f(\\tau + 1) = f(\\tau)$, and it also changes in a simple way under $\\tau \\mapsto -1/\\tau$.\nThese symmetries are so strong that, for each weight, the modular forms form a space of small dimension.\nThe [[Eisenstein series|EYREVY31BN]] $E_4(\\tau) = 1 + 240 \\sum_{n \\ge 1} \\sigma_3(n) q^n$ is an example of weight $4$.\nCoefficients of modular forms count things, such as the number of ways to write $n$ as a sum of squares.\n",
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