The 2014 paper of Cai, Bi and Luo proved mixed-species circular summation formulas for Jacobi theta functions — finite sums over knkn regularly shifted arguments of θ1aθ2b\theta_1^a\theta_2^b and of θ3aθ4b\theta_3^a\theta_4^b collapsing to a single θ3(z∣τ)\theta_3(z|\tau) — and supplied the Jacobi imaginary (modular) transformation τ→−1/τ\tau\to-1/\tau only for its pure-power theorems, dismissing the transformed counterparts of the two mixed theorems in Remark 1 as obtainable “the same way” and omitting them. Imaginary-transformed circular summations have been published only for the pure-power families, and mixed-product summations only in direct form; no published work supplies the transformed counterparts of the two mixed theorems. The problem is to derive and state explicitly both transformed identities, with the coefficients G12\mathscr{G}_{12} and G34\mathscr{G}_{34} given in the source paper’s dual form — as the modular image of the direct coefficients C12\mathscr{C}_{12} and C34\mathscr{C}_{34} and as explicit multiple series — together with the parity/divisibility constraints and sign factors under which each identity holds.

Background

Jacobi’s four theta functions, in the notation used throughout this literature, are defined for q=eiπτq=\mathrm{e}^{\mathrm{i}\pi\tau} with Im(τ)>0\mathrm{Im}(\tau)>0 and z∈Cz\in\mathbb{C} by

θ1(z∣τ)=−iq1/4∑m=−∞∞(−1)mqm(m+1)e(2m+1)iz,θ2(z∣τ)=q1/4∑m=−∞∞qm(m+1)e(2m+1)iz,\theta_1(z|\tau)=-\mathrm{i}q^{1/4}\sum_{m=-\infty}^{\infty}(-1)^m q^{m(m+1)}\mathrm{e}^{(2m+1)\mathrm{i}z},\qquad \theta_2(z|\tau)=q^{1/4}\sum_{m=-\infty}^{\infty}q^{m(m+1)}\mathrm{e}^{(2m+1)\mathrm{i}z}, θ3(z∣τ)=∑m=−∞∞qm2e2miz,θ4(z∣τ)=∑m=−∞∞(−1)mqm2e2miz.\theta_3(z|\tau)=\sum_{m=-\infty}^{\infty}q^{m^2}\mathrm{e}^{2m\mathrm{i}z},\qquad \theta_4(z|\tau)=\sum_{m=-\infty}^{\infty}(-1)^m q^{m^2}\mathrm{e}^{2m\mathrm{i}z}.

A circular summation formula expresses the sum of copies of a theta function (or of products of theta functions) evaluated at arguments shifted regularly around a period — “circularly” — as a single theta function times an explicit coefficient. The prototype goes back to Ramanujan; Chan, Liu and Ng (2006) proved the equivalence of the original claim with the theta-function form

∑k=0n−1qk2e2kiz θ3 n(z+kπτ ∣ nτ)=θ3(z∣τ) Fn(τ),\sum_{k=0}^{n-1}q^{k^2}\mathrm{e}^{2k\mathrm{i}z}\,\theta_3^{\,n}(z+k\pi\tau\,|\,n\tau)=\theta_3(z|\tau)\,F_n(\tau),

with FnF_n an explicit function of τ\tau (this is Theorem 1.8 as restated in the 2020 paper of Ge and Luo).

This equivalence triggered a family of generalizations. Zhou and Luo (2014) treated the pure θ4\theta_4-power family and also wrote out its image under the Jacobi imaginary transformation. Cai, Chen and Luo (2013) established mixed-product circular summations — products θiaθjb\theta_i^a\theta_j^b of two distinct species — for the pairs (1,3)(1,3), (1,4)(1,4), (2,3)(2,3), (2,4)(2,4). The source paper, “Some new circular summation formulas of theta functions” (Cai, Bi and Luo, 2014), closed the remaining two pairs with mixed θ1aθ2b\theta_1^a\theta_2^b (Theorem 4) and θ3aθ4b\theta_3^a\theta_4^b (Theorem 5) summations; later, Ge and Luo (2021) unified all six mixed pairs with general arguments, in direct form only.

The source paper’s two mixed theorems read as follows (the sums run over aa indices m1,…,mam_1,\ldots,m_a and bb indices n1,…,nbn_1,\ldots,n_b, with Σm=m1+⋯+ma\Sigma m=m_1+\cdots+m_a, Σn=n1+⋯+nb\Sigma n=n_1+\cdots+n_b, and per-index squares Σm2=m12+⋯+ma2\Sigma m^2=m_1^2+\cdots+m_a^2, Σn2=n12+⋯+nb2\Sigma n^2=n_1^2+\cdots+n_b^2).

Theorem 4 — for positive integers a,ba,b with aa and bb even, k=a+bk=a+b, and nn a positive integer:

∑s=0kn−1θ1a ⁣(zkn+ya+πskn ∣ τkn2)θ2b ⁣(zkn−yb+πskn ∣ τkn2)=C12 ⁣(a,b;yab,τkn2)θ3(z∣τ),\sum_{s=0}^{kn-1}\theta_1^{a}\!\left(\frac{z}{kn}+\frac{y}{a}+\frac{\pi s}{kn}\,\Big|\,\frac{\tau}{kn^{2}}\right)\theta_2^{b}\!\left(\frac{z}{kn}-\frac{y}{b}+\frac{\pi s}{kn}\,\Big|\,\frac{\tau}{kn^{2}}\right)=\mathscr{C}_{12}\!\left(a,b;\frac{y}{ab},\frac{\tau}{kn^{2}}\right)\theta_3(z|\tau),

where

C12(a,b;y,τ)=kn qk/4 ia∑m1,…,ma,n1,…,nb=−∞2(Σm+Σn)+k=0∞(−1)Σm qΣm2+Σn2+Σm+Σn eiy(2kΣm+ak).\mathscr{C}_{12}(a,b;y,\tau)=kn\,q^{k/4}\,\mathrm{i}^{a}\sum_{\substack{m_{1},\ldots,m_{a},\,n_{1},\ldots,n_{b}=-\infty\\2(\Sigma m+\Sigma n)+k=0}}^{\infty}(-1)^{\Sigma m}\,q^{\Sigma m^{2}+\Sigma n^{2}+\Sigma m+\Sigma n}\,\mathrm{e}^{\mathrm{i}y\left(2k\Sigma m+ak\right)}.

Theorem 5 — for positive integers a,ba,b with k=a+bk=a+b and bnbn even:

∑s=0kn−1θ3a ⁣(zkn+ya+πskn ∣ τkn2)θ4b ⁣(zkn−yb+πskn ∣ τkn2)=C34 ⁣(a,b;yab,τkn2)θ3(z∣τ),\sum_{s=0}^{kn-1}\theta_{3}^{a}\!\left(\frac{z}{kn}+\frac{y}{a}+\frac{\pi s}{kn}\,\Big|\,\frac{\tau}{kn^{2}}\right)\theta_{4}^{b}\!\left(\frac{z}{kn}-\frac{y}{b}+\frac{\pi s}{kn}\,\Big|\,\frac{\tau}{kn^{2}}\right)=\mathscr{C}_{34}\!\left(a,b;\frac{y}{ab},\frac{\tau}{kn^{2}}\right)\theta_{3}(z|\tau),

where

C34(a,b;y,τ)=kn∑m1,…,ma,n1,…,nb=−∞Σm+Σn=0∞(−1)Σn qΣm2+Σn2 e2kiy Σm.\mathscr{C}_{34}(a,b;y,\tau)=kn\sum_{\substack{m_{1},\ldots,m_{a},\,n_{1},\ldots,n_{b}=-\infty\\\Sigma m+\Sigma n=0}}^{\infty}(-1)^{\Sigma n}\,q^{\Sigma m^{2}+\Sigma n^{2}}\,\mathrm{e}^{2k\mathrm{i}y\,\Sigma m}.

The Jacobi imaginary transformation is the modular involution τ↦−1/τ\tau\mapsto-1/\tau acting on theta functions through the four standard identities (as stated in the papers of Zhou–Luo 2014 and Ge–Luo 2020):

θ1 ⁣(zτ ∣ −1τ)=−i (−iτ)1/2 eiz2/(πτ) θ1(z∣τ),θ2 ⁣(zτ ∣ −1τ)=(−iτ)1/2 eiz2/(πτ) θ4(z∣τ),\theta_1\!\left(\frac{z}{\tau}\,\Big|\,-\frac{1}{\tau}\right)=-\mathrm{i}\,(-\mathrm{i}\tau)^{1/2}\,\mathrm{e}^{\mathrm{i}z^{2}/(\pi\tau)}\,\theta_1(z|\tau),\qquad \theta_2\!\left(\frac{z}{\tau}\,\Big|\,-\frac{1}{\tau}\right)=(-\mathrm{i}\tau)^{1/2}\,\mathrm{e}^{\mathrm{i}z^{2}/(\pi\tau)}\,\theta_4(z|\tau), θ3 ⁣(zτ ∣ −1τ)=(−iτ)1/2 eiz2/(πτ) θ3(z∣τ),θ4 ⁣(zτ ∣ −1τ)=(−iτ)1/2 eiz2/(πτ) θ2(z∣τ),\theta_3\!\left(\frac{z}{\tau}\,\Big|\,-\frac{1}{\tau}\right)=(-\mathrm{i}\tau)^{1/2}\,\mathrm{e}^{\mathrm{i}z^{2}/(\pi\tau)}\,\theta_3(z|\tau),\qquad \theta_4\!\left(\frac{z}{\tau}\,\Big|\,-\frac{1}{\tau}\right)=(-\mathrm{i}\tau)^{1/2}\,\mathrm{e}^{\mathrm{i}z^{2}/(\pi\tau)}\,\theta_2(z|\tau),

so θ1\theta_1 and θ3\theta_3 map to themselves up to a Gaussian prefactor and a phase, while θ2\theta_2 and θ4\theta_4 are interchanged. Applied to a direct circular summation, it yields a genuinely new identity: in the published pure-family transforms (Theorems 6–8 of the source paper; Theorem 3.1 of Zhou–Luo 2014; Theorem 3.1 of Ge–Luo 2020) the left side becomes a weighted sum with τ\tau-scaled arguments — of the type qquadratic in k elinear in k and z θ(mz+yjπτ+mkπτ ∣ m2nτ)q^{\text{quadratic in }k}\,\mathrm{e}^{\text{linear in }k\text{ and }z}\,\theta(mz+y_j\pi\tau+mk\pi\tau\,|\,m^{2}n\tau) summed over kk — while the right side stays a single theta function of zz at modulus τ\tau (species fixed by parity), and the coefficient appears in dual form: both as the modular image of the direct coefficient and as an explicit multiple series.

For its three pure-power theorems the source paper carried out this program in full (Theorems 6–8, with coefficients G11\mathscr{G}_{11}, G22\mathscr{G}_{22}, G44\mathscr{G}_{44} in dual form). For the two mixed theorems it did not: Remark 1 states that the imaginary transformation formulas of Theorems 4 and 5 “may be obtained using the same way, we here omit them.” Under the transformation the θ2\theta_2-factors of Theorem 4 become θ4\theta_4-factors and the θ4\theta_4-factors of Theorem 5 become θ2\theta_2-factors, so the omitted formulas are mixed identities of a shape absent from the published literature.

Problem Statement

The problem is to write out, completely and explicitly, the two families of identities whose omission Remark 1 of Cai–Bi–Luo (2014) acknowledges: the Jacobi imaginary transformation (τ→−1/τ\tau\to-1/\tau) counterparts of Theorem 4 (mixed θ1aθ2b\theta_1^a\theta_2^b circular summation) and Theorem 5 (mixed θ3aθ4b\theta_3^a\theta_4^b circular summation).

Concretely, for each of the two theorems, an answer must provide:

  1. The transformed identity itself: an explicit summation formula in which the left side is built from the transformed factors — the θ2\theta_2-factors of Theorem 4 appearing as θ4\theta_4-factors and the θ4\theta_4-factors of Theorem 5 as θ2\theta_2-factors, with τ\tau-scaled arguments (of the mz+yjπτ+mkπτmz+y_j\pi\tau+mk\pi\tau type at a modulus of m2nτm^2n\tau type) and the Gaussian/phase weights the transformation generates — and the right side is a single theta function of zz at modulus τ\tau (species determined by parity) times a coefficient independent of zz, in the pattern set by the published pure-family transforms (Theorems 6–8 of the source paper; Theorem 3.1 of Zhou–Luo 2014 and of Ge–Luo 2020).

  2. The coefficient G12(a,b;y,τ)\mathscr{G}_{12}(a,b;y,\tau) (respectively G34\mathscr{G}_{34}) in dual form: both as the modular image of the direct coefficient C12\mathscr{C}_{12} (respectively C34\mathscr{C}_{34}) and as an explicit multiple series.

  3. The parity/divisibility constraints on aa, bb, nn under which each transformed identity holds, and the sign and phase factors appearing in each case (including the parity-determined choice of the right-side theta species).

The two identities, each complete in all three items enumerated above — the identity itself, the coefficient in both of its representations, and the parity/divisibility constraints with sign and phase factors — together constitute the completion boundary: an answer covering only one theorem, giving the coefficient in only one representation, omitting the parity/divisibility constraints or the sign and phase factors, or stating that the second follows “analogously” without writing it out, does not complete the problem. Both statements must be self-contained enough to be numerically evaluated from the statement alone.

References

  1. Heng Huat Chan, Zhi-Guo Liu, Say Tiong Ng, “Circular summation of theta functions in Ramanujan’s Lost Notebook”, Journal of Mathematical Analysis and Applications 316 (2006) 628–641. DOI: 10.1016/j.jmaa.2005.05.015, https://doi.org/10.1016/j.jmaa.2005.05.015 (its circular summation theorems appear as Theorems 1.7–1.9 of the Ge–Luo 2020 entry below).
  2. Jun-Ming Zhu, “An alternate circular summation formula of theta functions and its applications”, Applicable Analysis and Discrete Mathematics 6 (2012) 114–125. DOI: 10.2298/AADM120204004Z, https://doi.org/10.2298/AADM120204004Z.
  3. Yi Cai, Si Chen, Qiu-Ming Luo, “Some circular summation formulas for theta functions”, Boundary Value Problems 2013 (2013) 59. DOI: 10.1186/1687-2770-2013-59, https://doi.org/10.1186/1687-2770-2013-59.
  4. Yi Cai, Ya-Qing Bi, Qiu-Ming Luo, “Some new circular summation formulas of theta functions”, Integral Transforms and Special Functions 25 (2014) 497–507. DOI: 10.1080/10652469.2014.883388, https://doi.org/10.1080/10652469.2014.883388.
  5. Yun Zhou, Qiu-Ming Luo, “Circular summation formulas for theta function ϑ4(z|τ)”, Advances in Difference Equations 2014 (2014) 243. DOI: 10.1186/1687-1847-2014-243, https://doi.org/10.1186/1687-1847-2014-243.
  6. Qiu-Ming Luo, “A note for Ramanujan’s circular summation formula”, Integral Transforms and Special Functions 26 (2015) 567–585. DOI: 10.1080/10652469.2015.1028403, https://doi.org/10.1080/10652469.2015.1028403.
  7. Ji-Ke Ge, Qiu-Ming Luo, “Some Ramanujan-type circular summation formulas”, Advances in Difference Equations 2020 (2020) 690. DOI: 10.1186/s13662-020-03115-9, https://doi.org/10.1186/s13662-020-03115-9.
  8. Ji-Ke Ge, Qiu-Ming Luo, “Some extensions for Ramanujan’s circular summation formulas and applications”, The Ramanujan Journal 56 (2021) 491–518. DOI: 10.1007/s11139-020-00293-8, https://doi.org/10.1007/s11139-020-00293-8.