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Harmonic Maass Forms Summation Formula

Updated 29 September 2025
  • Harmonic Maass forms are nonholomorphic modular objects whose Fourier coefficients are connected via kernel-weighted summation identities.
  • The summation formulas employ analytic tools such as L-series, Mellin transforms, and modified Bessel functions to relate dual coefficients and arithmetic invariants.
  • Applications of these formulas include new identities for the partition function, Riesz means for cusp forms, and links to mock modular forms and singular moduli.

A summation formula for harmonic Maass forms is a transformation or explicit identity connecting a sum of the Fourier coefficients of a harmonic Maass form—often weighted by an analytic kernel such as a special function—with another sum, typically involving dual coefficients arising from an involutive automorphism (such as the Fricke operator), or arithmetic quantities like traces of singular moduli. Such formulas provide powerful analytic tools and deep arithmetic insight into modular objects of both integral and half-integral weight, and their paper involves techniques from the theory of LL-series, Mellin transforms, theta lifts, and regularization procedures.

1. Fourier Expansions and Harmonic Maass Forms

A harmonic Maass form ff of weight kk with respect to a congruence subgroup Γ0(N)\Gamma_0(N) (possibly with Nebentypus character) admits a Fourier expansion

f(z)=nn0c+(n)e2πinz+n>0c(n)Γ(1k,4πny)e2πinzˉ,f(z) = \sum_{n \geq -n_0} c^+(n) e^{2\pi i n z} + \sum_{n>0} c^-(n) \Gamma(1-k, 4\pi n y) e^{-2\pi i n \bar{z}},

where c+(n)c^+(n) and c(n)c^-(n) are the "holomorphic" and "non-holomorphic" Fourier coefficients, and Γ(s,x)\Gamma(s,x) is the incomplete Gamma function. The analytic and arithmetic paper of these coefficients is central to the understanding of harmonic Maass forms and their summation formulas (Diamantis et al., 26 Sep 2025, Diamantis et al., 2022).

2. L-series Machinery and Functional Equations

Recent advances leverage the theory of LL-series attached to harmonic Maass forms, defined by integrating the form against a family of suitable test functions φ\varphi: Lf(φ)=0f(iy)φ(y)dy.L_f(\varphi) = \int_{0}^{\infty} f(iy)\,\varphi(y)\,dy. For the Fourier expansion above, this LL-series can be written as

Lf(φ)=nn0c+(n)(Lφ)(2πn)+n>0c(n)0φ(t)()dt,L_f(\varphi) = \sum_{n \geq -n_0} c^{+}(n) (\mathcal{L}\varphi)(2\pi n) + \sum_{n>0} c^-(n)\int_{0}^{\infty}\varphi(t)(\ldots)dt,

where (Lφ)(s)=0estφ(t)dt(\mathcal{L}\varphi)(s) = \int_{0}^{\infty} e^{-st} \varphi(t)\,dt is the Laplace transform (Diamantis et al., 2021). Such LL-series possess functional equations mirroring modular transformation properties. For example, for a suitable φ\varphi and Fricke involution wNw_N one has

Lf(φ)=ikN1k/2LfkwN(φ2kwN),L_f(\varphi) = i^k N^{1-k/2} L_{f|_k w_N}(\varphi|_{2-k} w_N),

which forms the backbone of the kernel transformation in summation formulas.

3. The Summation Formula: Kernel-Weighted Sums and Bessel Transforms

A central result (Diamantis et al., 26 Sep 2025) is a transformation formula relating sums of Fourier coefficients of a harmonic Maass form weighted by special functions (typically modified Bessel functions) to sums over the dual coefficients associated to the Fricke involution. For a given C>0C>0 and XX, and with Dn=C+(2πn)/ND_n = C + (2\pi n)/\sqrt{N},

nn0c+(n)K0(2Dn(C+NX))±(non-holomorphic part)=ikCk/2nn0d+(n)(NX+Dn)k/2Kk(2C(Dn+NX))+(additional terms),\sum_{n \geq -n_0} c^+(n) K_0\big(2\sqrt{ D_n (C + \sqrt{N} X ) }\big) \pm (\text{non-holomorphic part}) = i^k C^{k/2} \sum_{n \geq -n_0} d^+(n) ( \sqrt{N} X + D_n )^{-k/2} K_k\big(2\sqrt{C(D_n + \sqrt{N} X)} \big) + (\text{additional terms}),

where KλK_\lambda denotes the modified Bessel function of the second kind, and d+(n)d^+(n) are the Fourier coefficients of fkwNf|_k w_N. Such formulas arise from explicit Mellin inversion identities: 0eaxb/xdxx=2K0(2ab),\int_{0}^{\infty} e^{-ax - b/x} \frac{dx}{x} = 2 K_0(2\sqrt{ab}), which naturally interpolate between exponential and oscillatory behaviors of modular sums. The choice of kernel (test function) is dictated by convergence and growth properties.

4. Applications: Partition Function and Classical Modular Forms

a) Partition Function

For the weakly holomorphic modular form f(z)=1/η(24z)f(z) = 1/\eta(24z), whose qq-expansion yields the partition numbers p(n)p(n),

1/η(24z)=q1/24n=0p(n)q24n,1/\eta(24z) = q^{-1/24} \sum_{n=0}^\infty p(n) q^{24 n},

the summation formula specializes to provide a new transformation identity for p(n)p(n) (Diamantis et al., 26 Sep 2025): n0p(n)K0(2(2πn+ε)(π/12+ε+24X))=(prefactor)n0p(n)(24X+2πn+ε)1/2e2(24X+2πn+ε)(π/12+ε),\sum_{n \geq 0} p(n) K_0 \big(2\sqrt{ (2\pi n + \varepsilon) (\pi/12 + \varepsilon + 24 X ) }\big) = (\text{prefactor}) \cdot \sum_{n \geq 0} p(n) (24 X + 2\pi n + \varepsilon)^{-1/2} e^{-2\sqrt{ (24 X + 2\pi n + \varepsilon ) ( \pi/12 + \varepsilon ) }}, with appropriate choices of constants. This formulation provides an alternative, kernel-weighted summation for the partition function, sharpening earlier algebraic and analytic trace formulas (Bruinier et al., 2011, Alfes, 2012).

b) Riesz Sums for Cusp Forms

For classical holomorphic cusp forms,

f(z)=n>0c(n)e2πinz,f(z) = \sum_{n > 0} c(n) e^{2\pi i n z},

the analogous machinery yields summation formulas for Riesz means, employing Kummer's confluent hypergeometric function M(s,k,x)M(s,k,x) and suitable kernel functions ψs(t)=1(0,1)(t)(1t)s1tks1/Γ(s)\psi_s(t) = \mathbf{1}_{(0,1)}(t)(1-t)^{s-1} t^{k-s-1}/\Gamma(s). These formulas allow extraction of asymptotic behaviors and exact relations between weighted sums of Fourier coefficients and special values of LL-series.

5. Generalizations and Associated Summation Phenomena

The kernel-based summation formula is not only limited to forms of integral weight but extends to half-integral weight, vector-valued harmonic Maass forms, and harmonic lifts. Extensions via theta lifts—using Kudla–Millson kernels or Shintani lift machinery—relate these summation formulas to traces of singular moduli, periods of modular functions, and algebraic objects in ring class fields (Bruinier et al., 2011, Alfes-Neumann et al., 2017, Alfes-Neumann et al., 2022). In many instances, such formulas lead to finite algebraic expressions for Fourier coefficients or CM-value traces, connecting automorphic analysis to deep arithmetic.

Regularized integrals and LL-series approaches provide further generalizations, enabling the formulation of summation identities for nonholomorphic forms, period integrals, and even for forms with nontrivial growth at cusps. For instance, the test-function formalism discussed in (Diamantis et al., 2022, Diamantis et al., 2021) leads to Voronoi-type, regularized summation formulas which are valid uniformly across a broad class of harmonic Maass forms.

6. Significance and Impact

Summation formulas for harmonic Maass forms unify several analytic, arithmetic, and geometric phenomena:

  • They provide explicit dualities between sums over Fourier coefficients and their images under modular involutions, with kernels encoding analytic or arithmetic information.
  • The use of LL-series and functional equations motivates analytic continuation and regularization techniques, extending the range of modular and Maass forms for which these formulas are valid.
  • Applications include nontrivial identities for the partition function, mock theta functions, and modular LL-values, with ramifications for combinatorics, the theory of traces of singular moduli, and special values of LL-functions.
  • The techniques generalize classical summation phenomena such as the Voronoi formula, and via Mellin inversion connect to spectral and representation-theoretic frameworks (Bringmann et al., 2016, Jääsaari et al., 2016).

The ongoing development of these methods continues to open new directions: from the algebraic classification of Fourier coefficients as traces (Alfes, 2012, Alfes-Neumann et al., 2022), to the construction of nonholomorphic lifts and regularized period formulas (Jeon et al., 2012, Alfes-Neumann et al., 2017), and their incorporation into the theory of automorphic LL-functions and periods.

7. Selected Table: Kernel Functions and Their Use in Summation Formulas

Kernel Type Formula Example Application
Modified Bessel KνK_\nu K0(2ab)K_0(2\sqrt{ab}), Kk(2ab)K_k(2\sqrt{ab}) Dual sum transformations
Laplace Transform (Lφ)(s)(\mathcal{L}\varphi)(s) LL-series and regularized sums
Confluent Hypergeometric MM M(s,k,x)M(s,k,x) Riesz means for cusp forms

Analytic kernels are carefully chosen to ensure convergence, Mellin-inversion accessibility, and compatibility with functional equations linking Fourier coefficients to their duals.


Summation formulas for harmonic Maass forms, primarily through kernel-weighted duality, Mellin and Laplace integral transforms, and LL-series functional equations, offer a rigorous and flexible toolkit for relating Fourier expansions and arithmetic invariants in the theory of automorphic forms. Their modern development, as exemplified in (Diamantis et al., 26 Sep 2025), systematically extends classical summation techniques, giving analytic control and explicit identities for a much broader class of modular objects.

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