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spt-Crank-Type Partitions Overview

Updated 10 July 2026
  • spt-Crank-Type partitions are partition-theoretic objects that refine the smallest-parts function by incorporating crank-like and rank-like statistics.
  • They utilize two-variable generating functions and Bailey pair techniques to uncover combinatorial, analytic, and arithmetic insights, including explicit congruences and asymptotics.
  • Recent developments extend the theory to overpartitions and restricted partitions, linking these refinements with mock modular forms and advanced moment-difference constructions.

Searching arXiv for recent and foundational papers on spt-crank-type partitions. Searching arXiv for “spt-crank partitions”, “higher order spt-functions”, and “spt-crank for overpartitions”. spt-crank-type partitions are partition-theoretic objects and refinements built to explain smallest-parts functions by means of crank-like or rank-like statistics. In the ordinary partition setting, the starting point is Andrews’ spt(n)\operatorname{spt}(n), the total number of occurrences of the smallest part in all partitions of nn; from there the subject expands to SS-partitions, marked and doubly marked partitions, overpartitions, Bailey-pair constructions, higher symmetrized moment differences, and related functions such as ospt(n)\operatorname{ospt}(n) and sptω(n)\operatorname{spt}_\omega(n). The literature uses the phrase in a broad sense: sometimes for combinatorial classes carrying an explicit spt-crank, sometimes for two-variable generating functions whose specialization at z=1z=1 yields an spt-type function, and sometimes for moment-difference constructions that generalize the basic relation between smallest-parts counts and rank/crank moments (Chen, 2017, Garvan et al., 2015).

1. Foundational framework

The basic smallest-parts function is defined by

spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),

where ns(λ)n_s(\lambda) is the multiplicity of the smallest part in a partition λ\lambda of nn. Its generating function is

nn0

The surrounding theory depends on the classical rank and crank distributions nn1 and nn2, together with their moments and symmetrized moments (Chen, 2017).

A central structural point is that spt-type functions are typically realized as differences between rank-like and crank-like quantities. In the ordinary partition case, the smallest-parts function is tied to second rank and crank moments. In higher-order and generalized settings, the same pattern persists: one introduces a refined crank statistic or a two-variable generating function, then proves that the resulting spt-type series is a moment difference, a rank–crank difference, or a root-of-unity specialization of a two-variable partition series (Garvan, 2010).

This framework supports several distinct but related enterprises. One is combinatorial: construct partition classes and a statistic whose residue classes split an spt-type function into equinumerous families. Another is analytic: derive generating functions, dissections, asymptotics, and modular or mock modular structure. A third is arithmetic: explain congruences of Ramanujan type and prove positivity or parity results.

2. Classical spt-crank for ordinary partitions

The original spt-crank of Andrews, Garvan, and Liang is defined on nn3-partitions. Let nn4 be the set of partitions into distinct parts and nn5 the set of all partitions. Then

nn6

For nn7, the spt-crank is

nn8

and the sign is nn9. The net count

SS0

refines SS1 and gives combinatorial explanations of the congruences modulo SS2 and SS3 (Chen et al., 2013).

A major development was the conversion of this signed vector-partition theory into signless ordinary partition models. Chen, Ji, and Zang introduced doubly marked partitions SS4, defined by Ferrers-diagram conditions SS5, SS6, and SS7. For such an object,

SS8

is the spt-crank. They proved that SS9 equals the number of doubly marked partitions of ospt(n)\operatorname{ospt}(n)0 with spt-crank ospt(n)\operatorname{ospt}(n)1, and established a bijection between marked partitions and doubly marked partitions, thereby solving the problem of defining the spt-crank directly on ordinary partition data (Chen et al., 2013).

The distribution theory of ospt(n)\operatorname{ospt}(n)2 is closely related to the cumulative distributions of the ordinary rank and crank. Andrews, Dyson, and Rhoades conjectured that ospt(n)\operatorname{ospt}(n)3 is unimodal; Chen and collaborators proved this by introducing the ospt(n)\operatorname{ospt}(n)4-Durfee rectangle symbol and constructing explicit injections. In that setting,

ospt(n)\operatorname{ospt}(n)5

so unimodality is equivalent to an inequality between cumulative rank and crank counts (Chen et al., 2013).

A further refinement is the “nearly equal distribution” theorem. For every ospt(n)\operatorname{ospt}(n)6, there is a reordering ospt(n)\operatorname{ospt}(n)7 of the partitions of ospt(n)\operatorname{ospt}(n)8 such that

ospt(n)\operatorname{ospt}(n)9

This gives a new combinatorial interpretation of

sptω(n)\operatorname{spt}_\omega(n)0

it counts those partitions sptω(n)\operatorname{spt}_\omega(n)1 for which sptω(n)\operatorname{spt}_\omega(n)2 (Chen et al., 2017).

3. Moment-difference theory and higher orders

A decisive extension came from the introduction of positive moments. For sptω(n)\operatorname{spt}_\omega(n)3,

sptω(n)\operatorname{spt}_\omega(n)4

Bringmann and Mahlburg proved that these two families are asymptotically equal, but that the crank moments are asymptotically larger: sptω(n)\operatorname{spt}_\omega(n)5 while

sptω(n)\operatorname{spt}_\omega(n)6

In particular, sptω(n)\operatorname{spt}_\omega(n)7 for sufficiently large sptω(n)\operatorname{spt}_\omega(n)8 and all sptω(n)\operatorname{spt}_\omega(n)9 (Bringmann et al., 2012).

The first positive-moment difference is the ospt-function,

z=1z=10

Andrews, Chan, and Kim gave it a combinatorial interpretation in terms of certain “even and odd strings” in partitions, ensuring z=1z=11 and weak monotonicity in z=1z=12. Bringmann and Mahlburg obtained its asymptotic behavior,

z=1z=13

and proved the parity relation

z=1z=14

They also determined when z=1z=15 is odd: precisely when z=1z=16 for some prime z=1z=17 with z=1z=18 (Bringmann et al., 2012).

Garvan’s higher-order theory packages these ideas in terms of symmetrized moments. For z=1z=19,

spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),0

where spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),1 and spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),2 are the spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),3-th symmetrized crank and rank moments. The associated generating function is a nested multiple series, and the difference admits a weighted combinatorial interpretation over partitions. This yields, for all spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),4 and spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),5,

spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),6

together with explicit congruences for spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),7, spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),8, and spt(n)=λP(n)ns(λ),\operatorname{spt}(n)=\sum_{\lambda\in P(n)} n_s(\lambda),9 (Garvan, 2010).

4. Overpartitions and other restricted partition classes

The spt-crank program extends naturally to overpartitions and related classes. In this setting one encounters ns(λ)n_s(\lambda)0, ns(λ)n_s(\lambda)1, ns(λ)n_s(\lambda)2, and ns(λ)n_s(\lambda)3, where the smallest part may be constrained by parity, overlining, or the requirement that odd parts not repeat. Bringmann, Lovejoy, and Osburn showed that the generating functions of these spt-overpartition functions are quasimock theta functions, and Jennings-Shaffer defined spt-cranks on vector partitions that explain their simple congruences (Garvan et al., 2013).

For overpartitions, the two-variable series

ns(λ)n_s(\lambda)4

play the role of spt-crank generating functions. They satisfy rank–crank difference identities of the form

ns(λ)n_s(\lambda)5

with analogous formulas for the other families. By specializing ns(λ)n_s(\lambda)6 to roots of unity and using Bailey’s Lemma together with overpartition rank-difference formulas, one obtains combinatorial refinements of congruences such as

ns(λ)n_s(\lambda)7

as well as equidistribution statements on marked overpartitions (Garvan et al., 2013).

A more specialized example is ns(λ)n_s(\lambda)8, the total number of occurrences of the smallest parts among overpartitions of ns(λ)n_s(\lambda)9 where the smallest part is even and not overlined. Jennings-Shaffer gave another spt-crank for this function using the λ\lambda0-rank and a residual crank, and proved a 3-dissection at λ\lambda1 in which the coefficients of λ\lambda2 and λ\lambda3 vanish. This yields a combinatorial refinement of

λ\lambda4

(Jennings-Shaffer, 2014).

The higher-order theory also has overpartition analogues. For overpartitions, overpartitions with smallest part even, and partitions with smallest part even and no repeated odd parts, the higher-order spt-functions are again defined as differences of symmetrized crank and rank moments, and each has an explicit multiple-sum generating function. In these settings the corresponding crank moments dominate the rank moments, yielding nonnegativity of the higher-order spt-type functions and new congruences (Jennings-Shaffer, 2014).

Family Statistic or series Representative property
Overpartitions λ\lambda5, λ\lambda6, λ\lambda7, λ\lambda8 Combinatorial refinements of simple mod λ\lambda9 and mod nn0 congruences
Overpartitions with even smallest part nn1-rank and residual crank 3-dissection explaining nn2 and nn3
Partitions without repeated odd parts nn4, nn5 Congruences derived from exact relations between rank and residual crank moments

For partitions without repeated odd parts, Jennings-Shaffer used quasimodular forms on nn6 to derive exact relations between the nn7-rank and three residual cranks. These identities imply congruences for nn8 and nn9, including

nn00

(Jennings-Shaffer, 2014).

5. Bailey pairs, generalized spt-crank-type families, and mock modularity

A large branch of the subject constructs spt-crank-type functions from Bailey pairs. For an appropriate Bailey pair nn01, Garvan and collaborators define

nn02

whose specialization nn03 is an spt-type generating function. In this framework the Bailey pairs nn04 yield both old and new spt-type functions, each admitting Ramanujan-type congruences explained by the two-variable crank series. The corresponding nn05 have representations as infinite products or as Hecke–Rogers-type double sums, and root-of-unity dissections identify vanishing coefficients that force congruences [(Garvan et al., 2015); (Jennings-Shaffer, 2014)].

A related extension uses conjugate Bailey pairs and two four-variable nn06-hypergeometric functions nn07 and nn08. Their specializations produce new spt-crank-type functions such as nn09, nn10, nn11, nn12, nn13, nn14, and nn15, together with mod nn16 and mod nn17 congruences. The same formalism also specializes to many previously known spt-crank-type functions, so nn18 and nn19 act as master templates for a substantial part of the theory (Jennings-Shaffer, 2015).

The function nn20 occupies a particularly explicit mock-theoretic niche. Here nn21 counts partitions of nn22 such that all odd parts are smaller than twice the smallest part, with

nn23

where nn24 is Ramanujan’s third order mock theta function. Garvan and Jennings-Shaffer introduced a crank nn25 whose residue classes explain

nn26

For fixed nn27, nn28 is asymptotically positive, and the differences nn29 have an alternating sign pattern for large nn30. The generating series nn31 is the holomorphic part of a weight nn32 harmonic weak Maass form (Jang et al., 2016).

This broad Bailey-pair literature makes clear that “spt-crank-type” is not restricted to a single combinatorial model. Rather, it denotes a recurrent mechanism: an spt-type function is embedded in a two-variable nn33-series, root-of-unity evaluations detect equidistribution, and the resulting dissections yield explicit congruences.

6. Arithmetic, finite analogues, equidistribution, and recent directions

The theory also admits finite analogues. For the restricted partition function nn34, where the largest part is at most nn35, Dixit and collaborators define

nn36

They introduce finite rank and crank generating functions on vector partitions, define finite moments nn37 and nn38, and prove the exact identity

nn39

As in the unrestricted case, one has

nn40

and the higher-even-moment analogue is conjectured (Dixit et al., 2018).

A different algebraic direction studies partition polynomials. Using equidistribution criteria, Bringmann, Gomez, Rolen, and Tripp proved that the spt-crank Laurent polynomials satisfy

nn41

and that the quotient coefficients are non-negative. As corollaries, one recovers

nn42

The same work shows that the roots of the principal spt-crank polynomials become equidistributed on the unit circle as nn43 (Folsom et al., 2022).

Bias phenomena among rank and crank classes also remain relevant. Bringmann and Pandey proved detailed inequalities among rank classes, crank classes, and nn44 modulo nn45, confirming Borozenets’ conjectures. The paper is not itself an spt-crank construction, but it supplies explicit orderings among residue classes that the authors describe as groundwork for analogous investigations of spt-crank-type distributions modulo nn46 (Bringmann et al., 2023). This suggests that the arithmetic study of residue-class biases can continue to feed into spt-refinement problems.

A recent higher-moment development concerns the fourth symmetrized crank. A smallest-parts function nn47 attached to the fourth symmetrized crank is constructed so that

nn48

and it satisfies

nn49

The paper also proves congruences such as

nn50

together with asymptotics showing that nn51 and nn52 have the same leading exponential growth (Patkowski, 8 Nov 2025).

Taken together, these developments show that spt-crank-type partitions form a research program rather than a single construction. Its recurring themes are explicit combinatorial models, two-variable generating functions, rank–crank differences, Bailey-pair machinery, modular and mock modular structures, and arithmetic refinement through congruences, parity, asymptotics, and equidistribution.

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