Matsuda (Osaka J. Math. 2020) derived closed polynomial differential systems for the level-three cubic theta functions a(q)a(q), b3(q)b^3(q), c3(q)c^3(q) together with the Eisenstein series E2(q)E_2(q) and E2(q3)E_2(q^3), and proved that the differential fields they generate under q d/dqq\,d/dq all coincide and contain Ramanujan's differential field C(E2,E4,E6)\mathbb{C}(E_2,E_4,E_6). At level two the corresponding structure is completely understood: Ohyama proved that Halphen's differential field is a finite extension of Ramanujan's field whose differential Galois group is the symmetric group S3S_3. The level-three analogue is open: determining the differential Galois group of K3=C⟨a,E2,b3⟩K_3=\mathbb{C}\langle a,E_2,b^3\rangle over Ramanujan's field. No determination of this group appears in the literature. Relevant context for the determination includes the degree-four covering X0(3)→X(1)X_0(3)\to X(1) of modular curves (Galois closure group PSL2(F3)≅A4\mathrm{PSL}_2(\mathbb{F}_3)\cong A_4), the nontrivial weights and characters of the generators, and the quasi-modular E2E_2.

Background

Let q=exp⁡(2πiτ)q=\exp(2\pi i\tau) with τ\tau in the upper half-plane, and let δ=q ddq=12πiddτ\delta=q\,\frac{d}{dq}=\frac{1}{2\pi i}\frac{d}{d\tau} be the natural derivation acting on qq-series. The classical Eisenstein series

E2(q)=1−24∑n≥1σ1(n)qn,E4(q)=1+240∑n≥1σ3(n)qn,E6(q)=1−504∑n≥1σ5(n)qn,E_2(q)=1-24\sum_{n\ge1}\sigma_1(n)q^n,\qquad E_4(q)=1+240\sum_{n\ge1}\sigma_3(n)q^n,\qquad E_6(q)=1-504\sum_{n\ge1}\sigma_5(n)q^n,

where σk(n)\sigma_k(n) denotes the sum of the kk-th powers of the positive divisors of nn, satisfy Ramanujan's system of ordinary differential equations

δE2=E22−E412,δE4=E2E4−E63,δE6=E2E6−E422.\delta E_2=\frac{E_2^2-E_4}{12},\qquad \delta E_4=\frac{E_2E_4-E_6}{3},\qquad \delta E_6=\frac{E_2E_6-E_4^2}{2}.

Here E4E_4 and E6E_6 are modular forms of weights 4 and 6 (a modular form of weight kk for a group Γ⊂SL2(Z)\Gamma\subset SL_2(\mathbb{Z}) is a holomorphic function on the upper half-plane with f(aτ+bcτ+d)=(cτ+d)kf(τ)f(\frac{a\tau+b}{c\tau+d})=(c\tau+d)^k f(\tau) for (abcd)∈Γ\begin{pmatrix}a&b\\c&d\end{pmatrix}\in\Gamma), while E2E_2 is only quasi-modular: it satisfies the weight-2 transformation law up to an additive correction. The differential field R=C⟨E2,E4,E6⟩\mathcal{R}=\mathbb{C}\langle E_2,E_4,E_6\rangle generated by these three functions under δ\delta is Ramanujan's differential field. Throughout, the level of a form refers to the smallest NN such that it is modular for the congruence subgroup Γ0(N)\Gamma_0(N) (matrices of SL2(Z)SL_2(\mathbb{Z}) whose lower-left entry is divisible by NN).

The level-two member of this hierarchy is governed by Jacobi's theta constants ϑ2,ϑ3,ϑ4\vartheta_2,\vartheta_3,\vartheta_4 (values at z=0z=0 of the Jacobi theta function), whose logarithmic derivatives give the solutions of Halphen's nonlinear system X′+Y′=2XYX'+Y'=2XY, Y′+Z′=2YZY'+Z'=2YZ, Z′+X′=2ZXZ'+X'=2ZX. Ohyama (1995) proved that Halphen's differential field is a finite algebraic extension of Ramanujan's differential field whose differential Galois group is the symmetric group S3S_3. Here the differential Galois group means the group of automorphisms of the extension that commute with the derivation (the Kolchin group); for a finite algebraic extension of differential fields this is a finite group, and in the modular setting it realizes the deck transformations of the underlying covering of modular curves — at level two, the covering X(2)→X(1)X(2)\to X(1) of compactified modular curves, whose deck group is the anharmonic group of permutations of the modular lambda function. For a finite algebraic extension of differential fields, the extension is called differential-Galois when the base field is the fixed field of the differential Galois group — equivalently, when the order of that group equals the degree of the extension. Ohyama's theorem is the level-two prototype of the problem considered here.

The level-three (cubic) member involves the Borwein cubic theta functions

a(q)=∑m,n∈Zqm2+mn+n2,b(q)=∑m,n∈Zω n−mqm2+mn+n2,c(q)=∑m,n∈Zq(n+13)2+(n+13)(m+13)+(m+13)2,a(q)=\sum_{m,n\in\mathbb{Z}}q^{m^2+mn+n^2},\qquad b(q)=\sum_{m,n\in\mathbb{Z}}\omega^{\,n-m}q^{m^2+mn+n^2},\qquad c(q)=\sum_{m,n\in\mathbb{Z}}q^{(n+\frac13)^2+(n+\frac13)(m+\frac13)+(m+\frac13)^2},

with ω=e2πi/3\omega=e^{2\pi i/3}, introduced in the cubic (signature-3) theory of the Borwein brothers and Garvan; they satisfy the cubic identity a3=b3+c3a^3=b^3+c^3 and the eta-quotient expressions b3(q)=(q;q)∞9(q3;q3)∞3b^3(q)=\frac{(q;q)_\infty^9}{(q^3;q^3)_\infty^3} and c3(q)=27q (q3;q3)∞9(q;q)∞3c^3(q)=27q\,\frac{(q^3;q^3)_\infty^9}{(q;q)_\infty^3}, where (q;q)∞=∏n≥1(1−qn)(q;q)_\infty=\prod_{n\ge1}(1-q^n) and η(τ)=q1/24(q;q)∞\eta(\tau)=q^{1/24}(q;q)_\infty is the Dedekind eta function. These are modular forms for Γ0(3)\Gamma_0(3): aa has weight 1 and transforms with the nontrivial Dirichlet character modulo 3 (the quadratic character χ−3\chi_{-3} with χ−3(1)=1\chi_{-3}(1)=1, χ−3(2)=−1\chi_{-3}(2)=-1, χ−3(3)=0\chi_{-3}(3)=0), while b3b^3 and c3c^3 have weight 3. Ohyama (2001) derived Halphen-type systems at level three from Picard-Fuchs equations of elliptic modular surfaces; Huber (2011) obtained the differential systems for the cubic theta functions; and Matsuda (2020) — the source paper — rederived and extended them using Farkas and Kra's theory of theta functions with rational characteristics: theta functions θ[ϵϵ′](z,τ)\theta\bigl[\begin{smallmatrix}\epsilon\\ \epsilon'\end{smallmatrix}\bigr](z,\tau) indexed by a characteristic (ϵ,ϵ′)(\epsilon,\epsilon'), whose values at z=0z=0 (theta constants) at rational characteristics generate modular forms of the corresponding level. Matsuda's Theorems 1.1 and 1.2 give the closed polynomial systems

δa=3a3+aE2−4b312,δE2=−9a4+8ab3+E2212,δb3=−a2b3+E2b34,\delta a=\frac{3a^3+aE_2-4b^3}{12},\quad \delta E_2=\frac{-9a^4+8ab^3+E_2^2}{12},\quad \delta b^3=\frac{-a^2b^3+E_2b^3}{4},

δa=−3a3+3aE2(q3)+4c312,δE2(q3)=−9a4+8ac3+9E2(q3)236,δc3=a2c3+3E2(q3)c34,\delta a=\frac{-3a^3+3aE_2(q^3)+4c^3}{12},\quad \delta E_2(q^3)=\frac{-9a^4+8ac^3+9E_2(q^3)^2}{36},\quad \delta c^3=\frac{a^2c^3+3E_2(q^3)c^3}{4},

and, at the heart of the present problem, the structural facts that the resulting differential fields coincide,

K3:=C⟨a,E2,b3⟩=C⟨a,E2⟩=C⟨a,E2(q3)⟩=C⟨a,b3⟩,K_3:=\mathbb{C}\langle a,E_2,b^3\rangle=\mathbb{C}\langle a,E_2\rangle=\mathbb{C}\langle a,E_2(q^3)\rangle=\mathbb{C}\langle a,b^3\rangle,

and that Ramanujan's field is contained in K3K_3, with E4E_4 and E6E_6 rationally expressible through aa and b3b^3 (so R⊂K3\mathcal{R}\subset K_3 and the extension is finite algebraic). Related systems were developed at level five by Mano and for the Hecke groups Γ0(N)\Gamma_0(N), N=2,3,4N=2,3,4, by Maier; Opanasenko and Ferapontov later gave a general framework of Lie-group-invariant defining equations for modular forms in which the level-three form aa appears as an example.

What no published work supplies is the group-theoretic analogue of Ohyama's level-two theorem for this level-three field. The naive guess — that the group should be read off from the covering X0(3)→X(1)X_0(3)\to X(1) of modular curves, a degree-4 cover whose Galois closure has deck group PSL2(F3)≅A4\mathrm{PSL}_2(\mathbb{F}_3)\cong A_4 — must be reconciled with the facts that the generators carry nontrivial weights and characters (so deck transformations act on them with weight factors and character signs, and a character extension of A4A_4, for instance related to SL2(F3)SL_2(\mathbb{F}_3), may occur) and that the base field contains the quasi-modular E2E_2. The actual group, the degree of the extension, and even whether the extension is differential-Galois are undetermined in the literature.

Problem Statement

Let δ=q ddq\delta=q\,\frac{d}{dq}, let R=C⟨E2(q),E4(q),E6(q)⟩\mathcal{R}=\mathbb{C}\langle E_2(q),E_4(q),E_6(q)\rangle be Ramanujan's differential field, and let

K3=C⟨a(q),E2(q),b3(q)⟩=C⟨a(q),E2(q)⟩=C⟨a(q),E2(q3)⟩=C⟨a(q),b3(q)⟩K_3=\mathbb{C}\langle a(q),E_2(q),b^3(q)\rangle=\mathbb{C}\langle a(q),E_2(q)\rangle=\mathbb{C}\langle a(q),E_2(q^3)\rangle=\mathbb{C}\langle a(q),b^3(q)\rangle

be the level-three differential field generated by the cubic theta functions together with the Eisenstein series. The equalities of these fields, the containment R⊂K3\mathcal{R}\subset K_3, and the closed polynomial differential systems satisfied by the triples (a,E2,b3)(a,E_2,b^3) and (a,E2(q3),c3)(a,E_2(q^3),c^3) (with c3=a3−b3∈K3c^3=a^3-b^3\in K_3) are established in the source paper; any of these generating sets may be used. The problem is to determine the differential-algebraic structure of K3K_3 as an extension of R\mathcal{R}: determine the group of differential automorphisms of K3K_3 over R\mathcal{R} — the automorphisms of K3K_3, or of its Galois closure if the extension is not normal, that fix R\mathcal{R} pointwise and commute with δ\delta. The answer must specify the isomorphism type of this finite group, the degree [K3:R][K_3:\mathcal{R}] (and the degree of the Galois closure), whether the extension is differential-Galois, and explicit generators of the group, each automorphism being described by the images it assigns to a chosen set of generators of K3K_3 (for instance aa and b3b^3, with c3=a3−b3c^3=a^3-b^3 and E2(q3)E_2(q^3) then determined through the field equalities above; elements of R\mathcal{R}, in particular E2(q)E_2(q), are fixed pointwise; in the non-normal case, automorphisms of the Galois closure that do not preserve K3K_3 are described instead by their images on a generating set of the closure) — in the way the anharmonic group S3S_3 permutes the level-two generators — together with a proof that no further differential automorphisms exist. This is the level-three analogue of Ohyama's theorem that the Halphen field extends Ramanujan's field with differential Galois group S3S_3.

References

  1. Kazuhide Matsuda, Differential equations involving cubic theta functions and Eisenstein series, Osaka Journal of Mathematics 57(3), 521-542 (2020); arXiv:1609.07481, https://arxiv.org/abs/1609.07481 (zbMATH Zbl 7224919)
  2. Yousuke Ohyama, Differential relations of theta functions, Osaka Journal of Mathematics 32(2), 431-450 (1995), doi:10.18910/8440, https://doi.org/10.18910/8440 (zbMATH Zbl 880180)
  3. Yousuke Ohyama, Differential equations for modular forms of level three, Funkcialaj Ekvacioj 44(3), 377-389 (2001), https://zbmath.org/2112767 (zbMATH Zbl 2112767)
  4. Tim Huber, Differential equations for cubic theta functions, International Journal of Number Theory 7(7), 1945-1957 (2011), doi:10.1142/S1793042111004873, https://doi.org/10.1142/S1793042111004873
  5. Toshiyuki Mano, Differential relations for modular forms of level five, Journal of Mathematics of Kyoto University 42(1), 41-55 (2002), doi:10.1215/kjm/1250284710, https://doi.org/10.1215/kjm/1250284710
  6. Robert S. Maier, Nonlinear differential equations satisfied by certain classical modular forms, Manuscripta Mathematica 134, 1-42 (2011), doi:10.1007/s00229-010-0378-9, https://doi.org/10.1007/s00229-010-0378-9
  7. J. M. Borwein, P. B. Borwein, F. G. Garvan, Some cubic modular identities of Ramanujan, Transactions of the American Mathematical Society 343, 35-47 (1994), doi:10.1090/s0002-9947-1994-1243610-6, https://doi.org/10.1090/s0002-9947-1994-1243610-6
  8. Hershel M. Farkas, Irwin Kra, Theta constants, Riemann surfaces and the modular group: an introduction with applications to uniformization theorems, partition identities and combinatorial number theory, Graduate Studies in Mathematics 37, American Mathematical Society, Providence, RI (2001), ISBN 978-0-8218-1392-8, https://bookstore.ams.org/gsm-37/
  9. Kazuhide Matsuda, Cubic theta functions and modular forms of level six, The Ramanujan Journal 62(2), 469-532 (2023); arXiv:1508.05838, https://arxiv.org/abs/1508.05838, doi:10.1007/s11139-023-00757-7
  10. Kazuhide Matsuda, Note on Halphen's system, The Ramanujan Journal 55(3), 873-917 (2021), doi:10.1007/s11139-021-00439-2, https://doi.org/10.1007/s11139-021-00439-2
  11. Kazuhide Matsuda, Fuchsian differential equations with modular forms, arXiv:2004.05152 (2020), https://arxiv.org/abs/2004.05152
  12. Stanislav Opanasenko, Evgeny V. Ferapontov, Defining differential equations for modular forms and Jacobi forms, arXiv:2303.17936 (2023), https://arxiv.org/abs/2303.17936
  13. Sujay K. Ashok, Dileep P. Jatkar, Madhusudhan Raman, Triangle groups: automorphic forms and nonlinear differential equations, SIGMA 16 (2020), 102, doi:10.3842/SIGMA.2020.102, https://doi.org/10.3842/SIGMA.2020.102
  14. Ahmed Sebbar, Finite and infinite order differential relations for theta functions, Milan Journal of Mathematics 84(2), 317-347 (2016), doi:10.1007/s00032-016-0261-6, https://doi.org/10.1007/s00032-016-0261-6
  15. Ahmed Sebbar, Oumar Wone, Anharmonic solutions to the Riccati equation and elliptic modular functions, Forum Mathematicum 30(2), 433-455 (2018), doi:10.1515/forum-2017-0025, https://doi.org/10.1515/forum-2017-0025