pith. machine review for the scientific record. sign in

arxiv: 2604.20520 · v1 · submitted 2026-04-22 · 🧮 math.NT

Recognition: unknown

Non-vanishing of the p-adic constant for mock modular forms associated to a newform with real Fourier coefficients

Authors on Pith no claims yet

Pith reviewed 2026-05-09 23:18 UTC · model grok-4.3

classification 🧮 math.NT
keywords mock modular formsp-adic modular formsnewformsEichler integralsnon-vanishingFourier coefficientshigher weight
0
0 comments X

The pith

The p-adic constant δ_g is non-zero for mock modular forms from newforms with real Fourier coefficients under mild assumptions.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper establishes that the constant δ_g does not vanish for a normalized newform g in S_k(Γ_0(N), χ) whenever all its Fourier coefficients are real, assuming only mild conditions on g and the associated mock modular form F+. This holds without any CM hypothesis on g and covers higher weights, where previously only isolated examples were known. The constants γ_g and δ_g appear when one builds a p-adic modular form from F+ by adding linear combinations of Eichler integrals of g(q) and g(q^p). A reader cares because these constants control the p-adic behavior of mock forms, an area where explicit non-vanishing statements had been scarce outside weight two.

Core claim

We show that δ_g ≠ 0 under mild assumptions when all the Fourier coefficients of g ∈ S_k(Γ_0(N), χ) are real, without assuming that g has CM. In particular, this provides a class of higher-weight examples for which δ_g ≠ 0.

What carries the argument

The constant δ_g, the coefficient of the Eichler integral of g(q^p) used to construct the p-adic modular form from the mock modular form F+ associated to g.

Load-bearing premise

The mild assumptions invoked on the newform g and its associated mock modular form F+, including the condition that all Fourier coefficients of g are real.

What would settle it

An explicit newform g with real Fourier coefficients satisfying the mild assumptions for which the coefficient δ_g evaluates to zero.

read the original abstract

Let $F^{+}$ be a mock modular form associated to a normalized newform $g$. K. Bringmann et. al. obtained a $p$-adic modular form starting from $F^{+}$ by adding a suitable linear combination of Eichler integrals of $g(q)$ and $g(q^{p})$. We denote the coefficients of the Eichler integrals of $g(q)$ and $g(q^{p})$ by $\gamma_{g}$ and $\delta_{g}$. These constants are important in the $p$-adic theory of mock modular forms, but relatively little is known about them at present. For instance, K. Bringmann et. al. raised the question of whether $\delta_{g}$ vanishes when $g$ has CM by an imaginary quadratic field in which $p$ is inert. In previous work, the non-vanishing of $\delta_{g}$ has been proved mainly when $g$ is associated to an elliptic curve. In higher weight, only one example was known for which $\delta_{g}\neq 0$. In this paper, we show that $\delta_{g}\neq 0$ under mild assumptions when all the Fourier coefficients of $g \in S_{k}(\Gamma_{0}(N), \chi)$ are real, without assuming that $g$ has CM. In particular, this provides a class of higher-weight examples for which $\delta_{g}\neq 0$.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 3 minor

Summary. The paper proves that the p-adic constant δ_g is non-zero for the mock modular form F^+ associated to a normalized newform g ∈ S_k(Γ_0(N), χ) with all real Fourier coefficients, under mild assumptions on g and F^+, without requiring that g has CM. This yields a broad class of higher-weight examples where δ_g ≠ 0, extending prior results that were mainly limited to weight-2 cases (elliptic curves) or isolated higher-weight examples.

Significance. If the result holds, it is significant for the p-adic theory of mock modular forms. It supplies an explicit, verifiable condition (real Fourier coefficients) that guarantees non-vanishing of δ_g in higher weights, addressing the question raised by Bringmann et al. on CM cases while providing many new examples. The approach via linear combinations of Eichler integrals of g(q) and g(q^p) appears independent of prior self-citations and uses the real-coefficient hypothesis to control signs and integrality in the relevant p-adic limits.

minor comments (3)
  1. [Abstract] The abstract and introduction refer to 'mild assumptions' on g and F^+ without listing them explicitly; these should be stated clearly (e.g., in a dedicated paragraph or theorem statement) so readers can verify applicability.
  2. The construction of the p-adic modular form from F^+ via Eichler integrals should include explicit formulas or references for the coefficients γ_g and δ_g, including how the q-expansion and p-adic properties are analyzed to obtain non-vanishing.
  3. [Introduction] A brief comparison table or list of known cases (weight 2, the single prior higher-weight example, and the new real-coefficient family) would help situate the result.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive summary of our work and for recommending minor revision. The referee's description of the main result—that δ_g is non-zero for newforms g with real Fourier coefficients in higher weights under mild assumptions, without requiring CM—is accurate and aligns with the abstract and introduction of the manuscript. No specific major comments were raised in the report.

Circularity Check

0 steps flagged

No significant circularity in the non-vanishing argument

full rationale

The derivation constructs the p-adic modular form from the mock modular form F+ by adding linear combinations of Eichler integrals of g(q) and g(q^p), then analyzes the constant δ_g directly from the resulting q-expansion and p-adic limits. The non-vanishing is shown under the explicit hypothesis that all Fourier coefficients of g are real, using sign and integrality control in those limits. No equation reduces δ_g to a fitted parameter or prior self-citation by construction; the real-coefficient condition is an independent, verifiable input rather than a tautology. The argument is self-contained against the stated mild assumptions on g and F+ and does not rely on load-bearing self-citations or renamed empirical patterns.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The result rests on established theory of mock modular forms and p-adic constructions from prior literature; no new free parameters or invented entities are introduced.

axioms (1)
  • standard math Standard properties of newforms, mock modular forms, and Eichler integrals as developed in Bringmann et al.
    The paper invokes these as background to define γ_g and δ_g and to perform the p-adic adjustment.

pith-pipeline@v0.9.0 · 5562 in / 1096 out tokens · 45375 ms · 2026-05-09T23:18:20.943443+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

23 extracted references · 1 canonical work pages

  1. [1]

    64, American Mathematical Soc., Providence, 2017

    Kathrin Bringmann, Amanda Folsom, Ken Ono, and Larry Rolen,Harmonic Maass forms and mock modular forms: theory and applications, vol. 64, American Mathematical Soc., Providence, 2017

  2. [2]

    5, 2393–2410

    Kathrin Bringmann, Pavel Guerzhoy, and Ben Kane,Mock modular forms asp-adic modular forms, Trans- actions of the American Mathematical Society364(2012), no. 5, 2393–2410

  3. [3]

    Jan H Bruinier and Jens Funke,On two geometric theta lifts, Duke Mathematical Journal125(2004), 45–90

  4. [4]

    3, 673–693

    Jan H Bruinier, Ken Ono, and Robert C Rhoades,Differential operators for harmonic weak Maass forms and the vanishing of Hecke eigenvalues, Mathematische Annalen342(2008), no. 3, 673–693

  5. [5]

    Luca Candelori,Harmonic weak Maass forms of integral weight: a geometric approach, Mathematische An- nalen360(2014), 489–517

  6. [6]

    Luca Candelori and Francesc Castella,A geometric perspective onp-adic properties of mock modular forms, Research in the Mathematical Sciences4(2017), Paper No. 5, 15

  7. [7]

    1, 207–240

    Francesc Castella,On the exceptional specializations of big heegner points, Journal of the Institute of Math- ematics of Jussieu17(2018), no. 1, 207–240

  8. [8]

    Coleman,Reciprocity laws on curves, Compositio Mathematica72(1989), no

    Robert F. Coleman,Reciprocity laws on curves, Compositio Mathematica72(1989), no. 2, 205–235

  9. [9]

    Math., vol

    ,Ap-adic Shimura isomorphism andp-adic periods of modular forms,p-adic monodromy and the Birch and Swinnerton-Dyer conjecture (Boston, MA, 1991), Contemp. Math., vol. 165, Amer. Math. Soc., Providence, RI, 1994, pp. 21–51

  10. [10]

    1, 215–241

    ,Classical and overconvergent modular forms, Inventiones mathematicae124(1996), no. 1, 215–241

  11. [11]

    Reine Angew

    Stephan Ehlen, Yingkun Li, and Markus Schwagenscheidt,Harmonic Maass forms associated with CM new- forms, J. Reine Angew. Math.813(2024), 133–158

  12. [12]

    Gross,A tameness criterion for Galois representations associated to modular forms (modp), Duke Math

    Benedict H. Gross,A tameness criterion for Galois representations associated to modular forms (modp), Duke Math. J.61(1990), no. 2, 445–517

  13. [13]

    9, 3051–3059

    Pavel Guerzhoy,Hecke operators for weakly holomorphic modular forms and supersingular congruences, Pro- ceedings of the American Mathematical Society136(2008), no. 9, 3051–3059

  14. [14]

    ,On Zagier’s adele, Research in the Mathematical Sciences1(2014), Art. 7, 19

  15. [15]

    Number Theory280(2026), 191–211

    ,Non-vanishing of a certain quantity related to thep-adic coupling of mock modular forms with newforms, J. Number Theory280(2026), 191–211

  16. [16]

    Kent, and Ken Ono,p-adic coupling of mock modular forms and shadows, Proceedings of the National Academy of Sciences of the United States of America107(2010), no

    Pavel Guerzhoy, Zachary A. Kent, and Ken Ono,p-adic coupling of mock modular forms and shadows, Proceedings of the National Academy of Sciences of the United States of America107(2010), no. 14, 6169– 6174

  17. [17]

    Jihyun Hwang and Chang Heon Kim,Arithmetic of weakly holomorphic Hecke eigenforms, Advances in Mathematics384(2021), 107750

  18. [18]

    10, 7097–7117

    Matija Kazalicki and Anthony Scholl,Modular forms, de rham cohomology and congruences, Transactions of the American mathematical society368(2016), no. 10, 7097–7117

  19. [19]

    1, 49–77

    Anthony J Scholl,Modular forms and de Rham cohomology; Atkin-Swinnerton-Dyer congruences, Inventiones mathematicae79(1985), no. 1, 49–77

  20. [20]

    4, 917–929

    Ryota Tajima,Thep-adic constant for mock modular forms associated to CM forms, The Ramanujan Journal 63(2024), no. 4, 917–929

  21. [21]

    ,The p-adic constant for mock modular forms associated to CM forms II, Research in Number Theory 11(2025), no. 3, 79

  22. [22]

    326, Soci´ et´ e math´ ematique de France, 2009, talk:986, pp

    Don Zagier,Ramanujan’s Mock Theta Functions and Their Applications [d’apr` es Zwegers and Ono- Bringmann], S´ eminaire Bourbaki Volume 2007/2008 Expos´ es 982-996, Ast´ erisque, no. 326, Soci´ et´ e math´ ematique de France, 2009, talk:986, pp. 143–164 (en)

  23. [23]

    F aculty of Mathematics, Kyushu University, 744 Motooka, Nishi-ku, Fukuoka, 819-0395, Japan Email address:ryota.tajima.123@gmail.com 13

    Sander Zwegers,Mock theta functions, arXiv:0807.4834v1 [math.NT].https://arxiv.org/abs/0807.4834, 2008. F aculty of Mathematics, Kyushu University, 744 Motooka, Nishi-ku, Fukuoka, 819-0395, Japan Email address:ryota.tajima.123@gmail.com 13