Dixit and Kumar (Math. Ann. 393 (2025), 667–696; arXiv:2411.06412) proved that for every positive integer ss the Jacobi theta function ∑n∈Zanqn2/(2s)\sum_{n\in\mathbb{Z}}a^{n}q^{n^{2}/(2s)} admits a Rogers–Ramanujan dissection: it equals a finite sum of ss products of pairs of generalized Rogers–Ramanujan functions, recovering Ramanujan's generalized modular relation from the Lost Notebook at s=2s=2. Their concluding section poses four open problems, which share a common objective — to extend and interpret this dissection theorem: (1) whether the identities, including the vanishing family (1.17), reflect an underlying physical phenomenon, inversion-type formula, or homogeneous system; (2) whether Ramanujan's companion identity (6.1) admits an ss-parameter extension analogous to (1.10); (3) whether dissections exist whose left-hand sides are finite sums of products of three or more generalized Rogers–Ramanujan functions; and (4) whether the series ∑m≥0qsm(m−1)/2+m(k+s/2)/(q)m\sum_{m\ge0}q^{sm(m-1)/2+m(k+s/2)}/(q)_m for parameter cases not covered by Bressoud–Santos–Mondek admit partition-theoretic interpretations. Adjacent work applies the s=2s=2 identity as a tool and extends (6.1) bilaterally in a different direction (references 2 and 3), but none of the four problems has been resolved.

Background

Fix a complex number qq with ∣q∣<1|q|<1 and use the standard qq-series notation (A)0=1(A)_0=1, (A)n=(A;q)n=(1−A)(1−Aq)⋯(1−Aqn−1)(A)_n=(A;q)_n=(1-A)(1-Aq)\cdots(1-Aq^{n-1}) for n≥1n\ge1, and (A)∞=(A;q)∞=lim⁡n→∞(A;q)n(A)_\infty=(A;q)_\infty=\lim_{n\to\infty}(A;q)_n. The Rogers–Ramanujan functions are the series G(q)=∑n≥0qn2/(q)nG(q)=\sum_{n\ge0}q^{n^{2}}/(q)_n and H(q)=∑n≥0qn2+n/(q)nH(q)=\sum_{n\ge0}q^{n^{2}+n}/(q)_n; the celebrated Rogers–Ramanujan identities rewrite them as infinite products, and they permeate number theory, combinatorics, and physics — for instance in Baxter's exactly solved lattice models such as the hard-hexagon model (a two-dimensional lattice gas with a nearest-neighbor exclusion rule, solved exactly by Baxter using the Rogers–Ramanujan identities), and in the framework of Rogers–Ramanujan-type identities and their arithmetic properties developed by Griffin, Ono and Warnaar. Mock theta functions are the qq-series of Ramanujan's last letter to Hardy, which behave like theta functions asymptotically at roots of unity but lack their modular transformation laws; they come in orders (third, fifth, seventh, ...). By a generalized Rogers–Ramanujan function one means any series of the form ∑n≥0anq(cn2+dn)/s/(bq)n\sum_{n\ge0}a^{n}q^{(cn^{2}+dn)/s}/(bq)_n with a,b∈Ca,b\in\mathbb{C}, a≠0a\ne0, c,d∈Rc,d\in\mathbb{R}, s∈Ns\in\mathbb{N}.

On page 27 of Ramanujan's Lost Notebook (the collection of his unpublished results rediscovered by George E. Andrews in 1976), Ramanujan claimed a generalized modular relation: for a∈C∖{0}a\in\mathbb{C}\setminus\{0\} and b∈Cb\in\mathbb{C},

∑m=0∞a−2mqm2(bq)m∑n=0∞anbnqn2/4(q)n+∑m=0∞a−2m−1qm2+m(bq)m∑n=0∞anbnq(n+1)2/4(q)n=1(bq)∞∑n=−∞∞anqn2/4−(1−b)∑n=1∞anqn2/4∑ℓ=0n−1bℓ(q)ℓ,\sum_{m=0}^{\infty}\frac{a^{-2m}q^{m^{2}}}{(bq)_{m}}\sum_{n=0}^{\infty}\frac{a^{n}b^{n}q^{n^{2}/4}}{(q)_{n}}+\sum_{m=0}^{\infty}\frac{a^{-2m-1}q^{m^{2}+m}}{(bq)_{m}}\sum_{n=0}^{\infty}\frac{a^{n}b^{n}q^{(n+1)^{2}/4}}{(q)_{n}}=\frac{1}{(bq)_{\infty}}\sum_{n=-\infty}^{\infty}a^{n}q^{n^{2}/4}-(1-b)\sum_{n=1}^{\infty}a^{n}q^{n^{2}/4}\sum_{\ell=0}^{n-1}\frac{b^{\ell}}{(q)_{\ell}},

proved by Andrews. Setting a=b=1a=b=1 and rescaling qq yields the modular relation G(q)G(q4)+qH(q)H(q4)=(−q;q2)∞2G(q)G(q^{4})+qH(q)H(q^{4})=(-q;q^{2})_{\infty}^{2}, and a=b=−1a=b=-1 yields a relation between two fifth-order mock theta functions and G(q)G(q), H(q)H(q). On page 26 of the Lost Notebook (Entry 7.2.4 in Andrews–Berndt's edition, Part II) Ramanujan claimed a companion identity (proved by Andrews), a difference of two products of theta functions and generalized Rogers–Ramanujan series:

∑n=−∞∞anqn2/4∑n=0∞(−a)nqn2/4(q)n−∑n=−∞∞(−a)nqn2/4∑n=0∞anqn2/4(q)n=2q1/4(q)∞∑m=0∞a−2m−1qm2+m(q)m,\sum_{n=-\infty}^{\infty}a^{n}q^{n^{2}/4}\sum_{n=0}^{\infty}\frac{(-a)^{n}q^{n^{2}/4}}{(q)_{n}}-\sum_{n=-\infty}^{\infty}(-a)^{n}q^{n^{2}/4}\sum_{n=0}^{\infty}\frac{a^{n}q^{n^{2}/4}}{(q)_{n}}=2q^{1/4}(q)_{\infty}\sum_{m=0}^{\infty}\frac{a^{-2m-1}q^{m^{2}+m}}{(q)_{m}},

whose special cases include two of Watson's identities connecting G(q)G(q), H(q)H(q) with third-order mock theta functions.

Dixit and Kumar generalized the page-27 identity to a parameter s∈Ns\in\mathbb{N} (their Theorem 1.1): for a∈C∖{0}a\in\mathbb{C}\setminus\{0\}, b∈Cb\in\mathbb{C},

∑k=0s−1{∑m=0∞a−sm−kq(sm+k)2/(2s)(bq)m∑n=0∞anbnqn(n+2js−2k)/(2s)(q)n}=1(bq)∞∑n=−∞∞anqn2/(2s)−(1−b)∑n=1∞anqn2/(2s)∑ℓ=0n−1bℓ(q)ℓ,\sum_{k=0}^{s-1}\left\{\sum_{m=0}^{\infty}\frac{a^{-sm-k}q^{(sm+k)^{2}/(2s)}}{(bq)_{m}}\sum_{n=0}^{\infty}\frac{a^{n}b^{n}q^{n(n+2js-2k)/(2s)}}{(q)_{n}}\right\}=\frac{1}{(bq)_{\infty}}\sum_{n=-\infty}^{\infty}a^{n}q^{n^{2}/(2s)}-(1-b)\sum_{n=1}^{\infty}a^{n}q^{n^{2}/(2s)}\sum_{\ell=0}^{n-1}\frac{b^{\ell}}{(q)_{\ell}},

where j=0j=0 if k=0k=0 and j=1j=1 otherwise. Since for b=1b=1 the right-hand side is (up to 1/(q)∞1/(q)_\infty) the Jacobi theta function ∑n∈Zanqn2/(2s)\sum_{n\in\mathbb{Z}}a^{n}q^{n^{2}/(2s)}, this represents a theta function as a finite sum of ss products of pairs of generalized Rogers–Ramanujan functions — a Rogers–Ramanujan dissection. The case s=2s=2 recovers Ramanujan's identity; s=1s=1 gives a generalization of the Jacobi triple product identity (the classical formula expanding a theta function as an infinite product); and for s>2s>2 the authors give asymptotic evidence that the identities transcend the modular world, so they cannot be expected to follow from modular-forms machinery. Letting a=−q−1/(2s)a=-q^{-1/(2s)} annihilates the theta term and yields the vanishing family (1.17)

∑k=0s−1{∑m=0∞(−1)sm−kq(sm+k)(sm+k+1)/(2s)(q)m∑n=0∞(−1)nqn(n+2js−2k−1)/(2s)(q)n}=0.\sum_{k=0}^{s-1}\left\{\sum_{m=0}^{\infty}\frac{(-1)^{sm-k}q^{(sm+k)(sm+k+1)/(2s)}}{(q)_{m}}\sum_{n=0}^{\infty}\frac{(-1)^{n}q^{n(n+2js-2k-1)/(2s)}}{(q)_{n}}\right\}=0.

Two further threads matter for the open problems. First, sums and differences of products of quadruples of Rogers–Ramanujan functions G(q)G(q), H(q)H(q) are known — in Robins' thesis, in recent work of Channabasavayya, Keerthana and Ranganatha, and of Gugg — and these sit inside Ramanujan's forty identities for G(q)G(q) and H(q)H(q) classified by Berndt et al.; since the pair-product relation G(q)G(q4)+qH(q)H(q4)=(−q;q2)∞2G(q)G(q^{4})+qH(q)H(q^{4})=(-q;q^{2})_{\infty}^{2} was a special case of Ramanujan's generalized relation, it is natural to ask whether the triple- and quadruple-product relations admit analogous generalizations. Second, Bressoud, Santos and Mondek proved that, for their parameter ranges, series of the shape ∑m≥0qℓm(m−1)/2+(linear in m)/(q)m\sum_{m\ge0}q^{\ell m(m-1)/2+\text{(linear in }m\text{)}}/(q)_m are generating functions of three infinite families of equinumerous restricted partitions; within the a=b=1a=b=1 dissection series

∑m=0∞qsm(m−1)/2+m(k+s/2)(q)m,s∈N, 0≤k≤s−1,\sum_{m=0}^{\infty}\frac{q^{sm(m-1)/2+m(k+s/2)}}{(q)_{m}},\qquad s\in\mathbb{N},\ 0\le k\le s-1,

Dixit and Kumar note that the cases with ss even and k≤s/2k\le s/2 fall under the Bressoud–Santos–Mondek theorem, while the remaining cases have no known partition-theoretic interpretation.

Problem Statement

Solve the four interlinked open problems posed at the end of Section 7 of Dixit and Kumar's paper on the Rogers–Ramanujan dissection of a theta function, which together ask for the completion of the theory of that dissection — its structural meaning, its extension to the companion identity and to multi-factor products, and its partition-theoretic content. The four parts are independent questions of the same program: a complete solution addresses all four, while an answer to any single part is a self-contained contribution to it. For (3), a proof in the triple case already answers the existence question; for (4), an interpretation of a single previously uncovered family of (s,k)(s,k) suffices.

(1) Structural interpretation. Does the ss-parameter family (1.10) — in particular its s=2s=2 case (1.1) together with the companion identity (6.1), which vaguely resemble a pair of inversion formulas — represent an underlying physical phenomenon or an inversion-type formula? Does the vanishing family (1.17) hint at some homogeneous system? That is, exhibit a well-defined physical or combinatorial model, or an inversion/homogeneous-system framework, whose exact analysis realizes these identities (in the way, for example, that the Rogers–Ramanujan identities are realized in Baxter's exactly solved lattice models).

(2) Companion-identity extension. Ramanujan's identity (1.1) was generalized to the ss-parameter family (1.10). Extend the companion identity (6.1) in the same manner: find, and prove, an ss-parameter family of identities (a finite sum of ss terms in the spirit of (1.10)) whose s=2s=2 case is (6.1), or show that such a family cannot exist.

(3) Multi-factor dissections. Do there exist analogues of (1.1), more generally of (1.10), in which the left-hand side is a finite sum of products of three or more generalized Rogers–Ramanujan functions — i.e., multi-factor (triple, quadruple, ...) Rogers–Ramanujan dissections of theta functions — and if so, what are their right-hand sides? (This is motivated by the known identities for sums and differences of products of quadruples of the Rogers–Ramanujan functions G(q)G(q), H(q)H(q) in Robins' thesis, Channabasavayya–Keerthana–Ranganatha's Theorem 3.1, and Gugg's Theorem 4.1, which generalize Ramanujan's forty identities; the authors suggest asymptotic analysis as the most promising search method.)

(4) Partition-theoretic content of the remaining cases. For the series ∑m=0∞qsm(m−1)/2+m(k+s/2)/(q)m\sum_{m=0}^{\infty}q^{sm(m-1)/2+m(k+s/2)}/(q)_{m} with s∈Ns\in\mathbb{N} and 0≤k≤s−10\le k\le s-1 occurring in Theorem 1.1 with a=b=1a=b=1: the cases with ss even and k≤s/2k\le s/2 are covered by the Bressoud–Santos–Mondek theorem, which exhibits three restricted-partition families with these series as generating functions. Extract partition-theoretic interpretations and combinatorial consequences for the remaining cases (ss odd, or ss even with k>s/2k>s/2) — e.g., restricted-partition classes, bijections, or arithmetic of coefficients.

References

  1. A. Dixit and G. Kumar, The Rogers–Ramanujan dissection of a theta function, Mathematische Annalen 393 (2025), no. 1, 667–696. DOI: 10.1007/s00208-025-03265-9 (preprint arXiv:2411.06412). https://doi.org/10.1007/s00208-025-03265-9
  2. N. H. Zhou, Theta functions and transformations of bilateral basic hypergeometric series, preprint (2026), arXiv:2605.05094 (v2). https://arxiv.org/abs/2605.05094
  3. A. Dixit, G. Kumar and A. Srivastava, Non-Rascoe partitions and a rank parity function associated to the Rogers–Ramanujan partitions, preprint (2025), arXiv:2508.04359. https://arxiv.org/abs/2508.04359
  4. D. M. Bressoud, J. P. O. Santos and P. Mondek, A family of partition identities proved combinatorially, The Ramanujan Journal 4 (2000), 311–315. DOI: 10.1023/A:1009805221257. https://doi.org/10.1023/A:1009805221257
  5. Channabasavayya, G. K. Keerthana and Ranganatha Dasappa, On further modular relations for the Rogers–Ramanujan functions, Indian Journal of Pure and Applied Mathematics 56 (2025), no. 1, 113–124. DOI: 10.1007/s13226-023-00458-3. https://doi.org/10.1007/s13226-023-00458-3
  6. C. Gugg, On conjectures of Koike and Somos for modular identities for the Rogers–Ramanujan functions, International Journal of Number Theory 17 (2021), no. 2, 435–472. DOI: 10.1142/S1793042120400138. https://doi.org/10.1142/S1793042120400138
  7. M. J. Griffin, K. Ono and S. O. Warnaar, A framework of Rogers–Ramanujan identities and their arithmetic properties, Duke Mathematical Journal 165 (2016), no. 8, 1475–1527. DOI: 10.1215/00127094-3449994. https://doi.org/10.1215/00127094-3449994
  8. B. C. Berndt, G. Choi, Y.-S. Choi, H. Hahn, B. P. Yeap, A. J. Yee, H. Yesilyurt and J. Yi, Ramanujan's forty identities for the Rogers–Ramanujan functions, Memoirs of the American Mathematical Society 188 (2007), no. 880, 96 pp. DOI: 10.1090/memo/0880. https://doi.org/10.1090/memo/0880
  9. R. J. Baxter, Exactly Solved Models in Statistical Mechanics, Academic Press, London–New York, 1982.