Abstract
Modular graph functions are SL(2, ℤ)-invariant functions associated with Feynman graphs of a two-dimensional conformal field theory on a torus of modulus τ. For one-loop graphs they reduce to real analytic Eisenstein series. We obtain the Fourier series, including the constant and non-constant Fourier modes, of all two-loop modular graph functions, as well as their Poincaré series with respect to Γ∞\\PSL(2, ℤ). The Fourier and Poincaré series provide the tools to compute the Petersson inner product of two-loop modular graph functions using Rankin-Selberg-Zagier methods. Modular graph functions which are odd under τ → − overline{tau} are cuspidal functions, with exponential decay near the cusp, and exist starting at two loops. Holomorphic subgraph reduction and the sieve algorithm, developed in earlier work, are used to give a lower bound on the dimension of the space mathfrak{A} w of odd two-loop modular graph functions of weight w. For w ≤ 11 the bound is saturated and we exhibit a basis for mathfrak{A} w.
Highlights
A modular graph function is a function associated to a certain Feynman graph for a twodimensional conformal field theory on a torus with complex structure τ
Modular graph functions are SL(2, Z)-invariant functions associated with Feynman graphs of a two-dimensional conformal field theory on a torus of modulus τ
Holomorphic subgraph reduction and the sieve algorithm, developed in earlier work, are used to give a lower bound on the dimension of the space Aw of odd two-loop modular graph functions of weight w
Summary
A modular graph function is a function associated to a certain Feynman graph for a twodimensional conformal field theory on a torus with complex structure τ. The Fourier and Poincare series expansions provide all the tools needed to evaluate integrals of two-loop modular graph functions over the fundamental domain of PSL(2, Z), as well as the Petersson inner product between modular graph functions, using the RankinSelberg-Zagier methods Some of these integrals are needed to evaluate the contributions to the genus-one string amplitudes which are analytic in the external momenta [2, 4]. Technical details of the calculations and some explicit formulas for complicated expansion coefficients are relegated to the appendices
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