Abstract
The word ‘modular’ refers to the moduli space of complex curves (= Riemann surfaces) of genus 1. Such a curve can be represented as ℂ/Λ where Λ ⊂ ℂ is a lattice, two lattices Λ1 and Λ2 giving rise to the same curve if Λ2 = λΛ1 for some non-zero complex number λ. (For properties of curves of genus 1, see the lectures of Cohen and Bost/Cartier in this volume.) A modular function assigns to each lattice Λ a complex number F (Λ) with F(Λ1) = F(Λ2) if Λ2 = λΛ1. Since any lattice Λ = ℤω1+ℤω2 is equivalent to a lattice of the form ℤτ+ℤ with τ (= ω1/ω2) a non-real complex number, the function F is completely specified by the values f(τ) = F(ℤτ + ℤ) with r in ℂ \ ℝ or even, since f(τ) = f(−τ), with τ in the complex upper half-plane ℌ = { τ ∈ ℂ ∣ J(τ) > 0}. The fact that the lattice Λ is not changed by replacing the basis {ω1, ω2} by the new basis aω1 + bω2, cω1 + dω2 (a, b, c, d ∈ ℤ, ad − bc = ±1) translates into the modular invariance property \( f\left( {\frac{{a\tau + b}} {{c\tau + d}}} \right) = f\left( \tau \right) \).
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© 1992 Springer-Verlag Berlin Heidelberg
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Zagier, D. (1992). Introduction to Modular Forms. In: Waldschmidt, M., Moussa, P., Luck, JM., Itzykson, C. (eds) From Number Theory to Physics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-02838-4_4
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DOI: https://doi.org/10.1007/978-3-662-02838-4_4
Publisher Name: Springer, Berlin, Heidelberg
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