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arXiv:2607.02433v1 [math.RT] 02 Jul 2026

Part bounds for the Sylow permutation characters of SnS_{n}

Lorenzo Vanzi Address: Dipartimento di Matematica e Informatica Ulisse Dini, Universita degli Studi di Firenze Email address: lorenzo.vanzi1@edu.unifi.it
Abstract.

We study the Sylow permutation character of the symmetric group at the prime 22 and prove some new bounds on the number of parts of partitions corresponding to its constituents.

1. Introduction

Let GG be a finite group, let pp be a prime and let PP be a Sylow pp-subgroup of GG. The study of the interplay between the representation theory of GG and that of its Sylow subgroups has been an active research theme for decades [Nav18]. The structure of the Sylow permutation character (1P)G(1_{P})\uparrow^{G} encodes a great deal of information about the algebraic structure of the group GG. For instance, the normality of PP in GG can be read off the irreducible constituents of (1P)G(1_{P})\uparrow^{G} [MN12, GLLV22]. Despite this, very little is known about the decomposition of (1P)G(1_{P})\uparrow^{G} in general. In this article we focus our attention on the case where G=SnG=S_{n} is a symmetric group. From now on we let Ωp(n)\Omega_{p}(n) be the subset of Irr(Sn)\mathrm{Irr}(S_{n}) consisting of all the irreducible constituents of (1P)Sn(1_{P})\uparrow^{S_{n}}. Since irreducible characters of SnS_{n} are naturally labelled by partitions of nn, it is convenient to think of Ωp(n)\Omega_{p}(n) as a subset of 𝒫(n)\mathcal{P}(n), the set of partitions of nn.

In [GL18] Giannelli and Law gave a complete description of Ωp(n)\Omega_{p}(n) for every odd prime pp. In subsequent work, again considering only odd primes, they extended this analysis and described the irreducible constituents of θSn\theta\uparrow^{S_{n}}, for every θIrr(P)\theta\in\mathrm{Irr}(P) [GL25]. It is surprising that, despite the amount of information accumulated for odd primes, very little is known for the prime p=2p=2.

The aim of this note is to start the investigation of the set Ω2(n)\Omega_{2}(n). In order to present our main result, we briefly introduce some notation. Let (n)\mathcal{H}(n) be the set of hook partitions of nn. Namely, partitions of the form (nx,1x)(n-x,1^{x}), for some 0xn10\leq x\leq n-1. An easy consequence of [Gia17] is the complete description of the set Ω2(n)(n)\Omega_{2}(n)\cap\mathcal{H}(n). For this reason, here we focus on non-hook partitions. With this in mind, the question we ask ourselves is the following one: what is the maximal number \ell\in\mathbb{N} such that every non-hook partition with at most \ell parts lies in Ω2(n)\Omega_{2}(n)? We call Δ(n,k)\Delta(n,k) the subset of 𝒫(n)(n)\mathcal{P}(n)\smallsetminus\mathcal{H}(n) consisting of partitions with at most kk parts. The main result of this paper is Theorem 4.3 below, where for every nn we determine the maximal \ell such that Δ(n,)Ω2(n)\Delta(n,\ell)\subseteq\Omega_{2}(n). Ignoring a few exceptions for small values of nn, our main result can be stated as follows.

Theorem A.

Let nn\in\mathbb{N} and let us assume that n11n\geq 11. Let n=2a1+2a2++2atn=2^{a_{1}}+2^{a_{2}}+\cdots+2^{a_{t}} be its binary expansion, where a1>a2>>at0a_{1}>a_{2}>\cdots>a_{t}\geq 0. Then

Δ(n,k)Ω2(n)if and only ifka1+t1.\Delta(n,k)\subseteq\Omega_{2}(n)\ \text{if and only if}\ k\leq a_{1}+t-1.

Theorem A shows that the irreducible character corresponding to any non-hook partition with few parts is an irreducible constituent of the 22-Sylow permutation character. This result extends the analysis of the restriction to Sylow 22-subgroups previously performed in [Gia17] and [GV24]. We conclude by mentioning that we also prove a complementary result to Theorem A. More precisely, in Proposition 2.6 we show that the maximum number of parts of a partition in Ω2(n)\Omega_{2}(n) is n2\lceil\frac{n}{2}\rceil. This result may be already known to experts, but we were not able to find a proof of it in the literature.

Acknowledgments

The author thanks Eugenio Giannelli for suggesting this research project and for his invaluable help with the manuscript.

2. Background and Notation

In this section we will establish notation and present some preliminary results required for the proofs in this paper.

2.1. Partitions and characters of SnS_{n}

The reader will most likely be familiar with the following definitions, but we will recall them for the sake of clarity. Let nn be a positive integer. A partition of nn is a sequence λ=(λ1,,λt)\lambda=(\lambda_{1},\,\ldots,\,\lambda_{t}) of non-increasing positive integers such that i=1tλi=n\sum_{i=1}^{t}\lambda_{i}=n. We may sometimes write λs\lambda_{s} with s>ts>t, in this case the number is zero. We use 𝒫(n)\mathcal{P}(n) to denote the set of all partitions of nn. The Young diagram (or diagram) of a partition λ\lambda is the set

[λ]:={(i,j)×|1iand1jλi}.[\lambda]:=\{(i,j)\in\mathbb{N}\times\mathbb{N}\,|\hskip 5.69046pt1\leq i\hskip 5.69046pt\text{and}\hskip 5.69046pt1\leq j\leq\lambda_{i}\}.

The elements of [λ][\lambda] are called cells or boxes, and the two indices are respectively the row index and column index. Given a partition λ\lambda, the symbol λ\lambda^{\prime} will denote the conjugate partition, which is to say the partition whose diagram is obtained by swapping the coordinates of [λ][\lambda]. Note that λ1\lambda^{\prime}_{1} coincides with the number of parts of λ\lambda. The (i,j)(i,j)-hook of a partition λ\lambda is the subset of [λ][\lambda] defined as follows:

Hij(λ):={(s,t)[λ]|s=iandtj,ort=jandsi}.H_{ij}(\lambda):=\{(s,t)\in[\lambda]\,|\hskip 5.69046pts=i\hskip 5.69046pt\text{and}\hskip 5.69046ptt\geq j,\text{or}\hskip 5.69046ptt=j\hskip 5.69046pt\text{and}\hskip 5.69046pts\geq i\}.

A hook partition is a partition λ\lambda such that [λ]=H11(λ)[\lambda]=H_{11}(\lambda). The set of all hook partitions of nn will be written (n)\mathcal{H}(n). We will also use the following nonstandard definition: we say that λ\lambda is an almosthookalmost-hook partition if [λ]H11(λ)[\lambda]\setminus H_{11}(\lambda) has just one element. We will use 𝒜(n)\mathcal{AH}(n) to denote the set of all almost-hook partitions of nn.
It is a well known fact (e.g. [Jam78]) that the simple Sn\mathbb{C}S_{n}-modules up to isomorphism are the Specht modules indexed by partitions of nn. For λ𝒫(n)\lambda\in\mathcal{P}(n) we will use SλS^{\lambda} to denote the corresponding Specht module, and χλ\chi^{\lambda} the character corresponding to such module. We will recall the structure of these modules briefly, since it will be used in the next subsection. If λ𝒫(n)\lambda\in\mathcal{P}(n), a λ\lambda-tableau is a bijection [λ]{1,,n}[\lambda]\rightarrow\{1,\ldots,\,n\}. SnS_{n} acts naturally on the set of λ\lambda-tableaux. Let tt be a λ\lambda-tableau, RtR_{t} and CtC_{t} denote the subgroups of SnS_{n} that stabilize the rows and columns of tt respectively. We define an equivalence relation by tst\sim s if s=tτs=t\tau for some τRt\tau\in R_{t}. The equivalence class of tt is denoted by {t}\{t\}, and this is called a λ\lambda-tabloid. SnS_{n} acts naturally on the set of λ\lambda-tabloids. We call the permutation module of SnS_{n} over this set MλM^{\lambda}. The Specht module SλS^{\lambda} is the submodule of MλM^{\lambda} spanned by the λ\lambda-polytabloids: the elements of the form σCtsign(σ){t}σ\sum_{\sigma\in C_{t}}sign(\sigma)\{t\}\sigma where tt is a λ\lambda-tableau.
Another fundamental result in the representation theory of symmetric groups, which will be essential in almost all the proofs in this paper, is the Littlewood-Richardson Rule. To state it we will need some extra notation. Let n>mn>m be positive integers. Let λ𝒫(n)\lambda\in\mathcal{P}(n) and μ𝒫(m)\mu\in\mathcal{P}(m). We say that μ\mu is a subpartition of λ\lambda if [μ][λ][\mu]\subset[\lambda]. If μ\mu is a subpartition of λ\lambda we define the following set:

[λμ]:=[λ][μ].[\lambda\setminus\mu]:=[\lambda]\setminus[\mu].

This is known as a skew diagram. A sequence of positive integers 𝒞=(c1,,cn)\mathcal{C}=(c_{1},\ldots,c_{n}) is said to have weight λ\lambda if

λk=|{j:cj=k}|\lambda_{k}=|\{j:\hskip 5.69046ptc_{j}=k\}|

for all k1k\geq 1. An element cjc_{j} in the sequence is said to be good if cj=1c_{j}=1 or

|{i<j:ci=cj}|<|{i<j:ci=cj1}|.|\{i<j:\hskip 5.69046ptc_{i}=c_{j}\}|<|\{i<j:\hskip 5.69046ptc_{i}=c_{j}-1\}|.

If every element in the sequence is good we say that the sequence is good.
If n>mn>m are positive integers, we may identify Sm×SnmS_{m}\times S_{n-m} with any subgroup of SnS_{n} obtained as the direct product of the symmetric group acting on a subset of {1,,n}\{1,\ldots,\,n\} of cardinality mm and the symmetric group acting on its complement (these are called Young subgroups, and from now on when we write Sm×SnmSnS_{m}\times S_{n-m}\leq S_{n} it will always be a group of this form). The Littlewood-Richardson Rule allows for the construction of the restrictions of characters of SnS_{n} to Sm×SnmS_{m}\times S_{n-m} and inductions from these subgroups to SnS_{n}.

Theorem 2.1 (Littlewood-Richardson Rule).

Let n>mn>m be positive integers. Let μ𝒫(m)\mu\in\mathcal{P}(m) and ν𝒫(nm)\nu\in\mathcal{P}(n-m). Consider χμ×χνIrr(Sm×Snm)\chi^{\mu}\times\chi^{\nu}\in\mathrm{Irr}(S_{m}\times S_{n-m}). Then we have:

(χμ×χν)Sn=λ𝒫(n)cμνλχλ(\chi^{\mu}\times\chi^{\nu})\uparrow^{S_{n}}=\sum_{\lambda\in\mathcal{P}(n)}c^{\lambda}_{\mu\nu}\chi^{\lambda}

where cμνλc^{\lambda}_{\mu\nu} is the number of ways of filling [λμ][\lambda\setminus\mu] with positive numbers such that:
(i) the sequence obtained reading the numbers from right to left, top to bottom is a good sequence of weight ν\nu;
(ii) the numbers are strictly increasing along the columns from top to bottom;
(iii) the numbers are weakly increasing along the rows from left to right.

For a proof see for example [Jam78, The Littlewood-Richardson rule]. We refer to a filling of [λμ][\lambda\setminus\mu] of the type above as a Littlewood-Richardson filling of [λμ][\lambda\setminus\mu] of weight ν\nu. The above result shows that to prove that [(χμ×χν)Sn,χλ]0[(\chi^{\mu}\times\chi^{\nu})\uparrow^{S_{n}},\,\chi^{\lambda}]\neq 0, it suffices to find a Littlewood-Richardson (we will often abbreviate L-R) filling of [λμ][\lambda\setminus\mu] of weight ν\nu. This will be used many times in this paper. Let us also highlight two simple but useful facts: by swapping mm and nmn-m we see that if cμνλ0c^{\lambda}_{\mu\nu}\neq 0 then ν\nu is also a subpartition of λ\lambda; furthermore, in this case we have that λ1μ1+ν1\lambda_{1}\leq\mu_{1}+\nu_{1} and λ1μ1+ν1\lambda^{\prime}_{1}\leq\mu^{\prime}_{1}+\nu^{\prime}_{1}. And finally, let us state a simple to prove combinatorial remark, that will be used repeatedly in the sections below.

Remark 2.2.

Let n>mn>m be positive integers. Let λ𝒫(n)\lambda\in\mathcal{P}(n) and μ𝒫(m)\mu\in\mathcal{P}(m), such that μ\mu is a subpartition of λ\lambda; then the filling of [λμ][\lambda\setminus\mu] given by the top to bottom numbering of the boxes of each column is a Littlewood-Richardson filling.

In the following figure we give an example of this filling for the sake of clarity.

    ×\times   ×\times   ×\times   ×\times   ×\times   11   11        ×\times   ×\times   ×\times   ×\times   ×\times   22        ×\times   ×\times   ×\times   11   11   33        11   11        22   

Here λ=(7, 62, 2, 1)\lambda=(7,\,6^{2},\,2,\,1), μ=(52, 3)\mu=(5^{2},\,3) and the weight of the filling is (6, 2, 1)(6,\,2,\,1).

2.2. The Sylow Permutation Character

Let nn be a positive integer, we define the following sets:

Ωp(n):={λ𝒫(n)|[χλ,(1Pn)Sn]0}\Omega_{p}(n):=\{\lambda\in\mathcal{P}(n)\,|\hskip 5.69046pt[\chi^{\lambda},\,(1_{P_{n}})\uparrow^{S_{n}}]\neq 0\}

where PnP_{n} is a Sylow pp-subgroup of SnS_{n}. Clearly Ωp(n)\Omega_{p}(n) does not depend on the choice of the Sylow pp-subgroup. The character (1Pn)Sn(1_{P_{n}})\uparrow^{S_{n}} is called a Sylow permutation character, and its significance and the reasons for trying to find its decomposition have been touched on in the introduction. As has been said there, the set Ωp(n)\Omega_{p}(n) has been determined in its entirety in [GL18, Theorem A], when pp is odd. In this paper we focus instead on the much more irregular Ω2(n)\Omega_{2}(n), which still elude a full description.
We will now fix a particular Sylow 22-subgroup of SnS_{n} for each nn. This will allow us to prove two interesting facts about Ω2(n)\Omega_{2}(n) before even reducing the problem using Clifford Theory. Both these results may already be known to experts, but we were not able to find proofs of them in the literature. For any k0k\geq 0 we define P2kP_{2^{k}} as the Sylow 22-subgroup of S2kS_{2^{k}} generated by the elements: (1,2),(1,3)(2,4),,(1,2k1+1)(2k1,2k)(1,2),(1,3)(2,4),\ldots,(1,2^{k-1}+1)\cdots(2^{k-1},2^{k}). Let n>0n>0 be an integer, and n=2a1+2a2++2atn=2^{a_{1}}+2^{a_{2}}+\cdots+2^{a_{t}} its binary expansion, with a1>>ata_{1}>\cdots>a_{t}. We define PnP_{n} as the Sylow 22-subgroup of SnS_{n} obtained as the product of the natural embeddings of the subgroups P2akP_{2^{a_{k}}} in S{m+1,,m+2ak}S_{\{m+1,\ldots,\,m+2^{a_{k}}\}} (the symmetric group acting on the set {m+1,,m+2ak}\{m+1,\ldots,\,m+2^{a_{k}}\}) where m=2a1++2ak1m=2^{a_{1}}+\cdots+2^{a_{k-1}}. With this notation fixed, we may observe that (2k+1,2k+2)Pn(2k+1,2k+2)\in P_{n} for all k0k\geq 0 such that 2k+2n2k+2\leq n, and that PnP_{n} stabilizes the set {{2k+1, 2k+2}:22k+2n}\{\{2k+1,\,2k+2\}:\hskip 5.69046pt2\leq 2k+2\leq n\}.
We will use the structure of the Specht modules to prove the following two results, so we will need to translate the character theoretic condition for λΩ2(n)\lambda\in\Omega_{2}(n) into one that can be visualized in SλS^{\lambda}. This is done in the following lemma.

Lemma 2.3.

Let n>0n>0 be an integer, and λ𝒫(n)\lambda\in\mathcal{P}(n). Then λΩ2(n)\lambda\in\Omega_{2}(n) if and only if there exists a λ\lambda-tableau tt such that πPnetπ0\sum_{\pi\in P_{n}}e_{t}\pi\neq 0.

Proof.

The condition [χλPn, 1Pn]0[\,\chi^{\lambda}\downarrow_{P_{n}},\,1_{P_{n}}]\,\neq 0 is equivalent to

vSλ{0}πPnvπ=v.\exists v\in S^{\lambda}\setminus\{0\}\hskip 5.69046pt\forall\pi\in P_{n}\hskip 5.69046ptv\pi=v.

Since char()=0\mathrm{char}(\mathbb{C})=0, this in turn is equivalent to

wSλπPnwπ0.\exists w\in S^{\lambda}\hskip 5.69046pt\sum_{\pi\in P_{n}}w\pi\neq 0.

Since SλS^{\lambda} is spanned by the λ\lambda-polytabloids this last condition is equivalent to asking that there exist a λ\lambda-tableau tt such that πPnetπ0\sum_{\pi\in P_{n}}e_{t}\pi\neq 0. ∎

If all the parts of the partition are even, then it is easy to find such a tableau. This is the first result, and it will be used in the proofs leading to the main theorem.

Proposition 2.4.

Let n>0n>0 be an integer and λ𝒫(2n)\lambda\in\mathcal{P}(2n) a partition whose parts are all even, then λΩ2(2n)\lambda\in\Omega_{2}(2n).

Proof.

We will prove that the λ\lambda-tableau obtained by numbering the cells of [λ][\lambda] from left to right, top to bottom satisfies the condition in Lemma 2.3. Let tt be this λ\lambda-tableau. We have

πPnetπ=πPnσCtsign(σ){t}σπ.\sum_{\pi\in P_{n}}e_{t}\pi=\sum_{\pi\in P_{n}}\sum_{\sigma\in C_{t}}sign(\sigma)\{t\}\sigma\pi.

We will show that the coefficient of {t}\{t\} is positive. This coefficient is π,σsign(σ)\sum_{\pi,\sigma}sign(\sigma), where the sum is over all πPn\pi\in P_{n} and σCt\sigma\in C_{t} such that {t}σπ={t}\{t\}\sigma\pi=\{t\}, or equivalently {t}σ={t}π1\{t\}\sigma=\{t\}\pi^{-1}. If σ\sigma and π\pi satisfy this condition, then sign(σ)=1sign(\sigma)=1. This is because PnP_{n} stabilizes the set {{2k+1, 2k+2}:0kn1}\{\{2k+1,\,2k+2\}:\hskip 5.69046pt0\leq k\leq n-1\}, so for all such kk, if 2k+12k+1 is in a certain row of {t}π1\{t\}\pi^{-1} then 2k+22k+2 is in that same row (because this condition is true for {t}\{t\}). Any σCt\sigma\in C_{t} is the product of disjoint permutations acting on the individual columns. Since {t}σ={t}π1\{t\}\sigma=\{t\}\pi^{-1}, the previous condition tells us that the permutation acting on the column 2j+22j+2 has the same cyclic type as the one acting on the column 2j+12j+1, since each couple of adjacent elements in these columns of {t}\{t\} is of the type {2k+1, 2k+2}\{2k+1,\,2k+2\}. This means that sign(σ)=1sign(\sigma)=1. Since 1PnCt1\in P_{n}\cap C_{t} the coefficient of {t}\{t\} is at least one. ∎

The next result we will prove is the result alluded to in the introduction as complementary to the main theorem. In this case we want to prove that certain partitions are not in Ω2(n)\Omega_{2}(n). This can be achieved with the following lemma.

Lemma 2.5.

Let n>0n>0 be an integer. If λ𝒫(n)\lambda\in\mathcal{P}(n) is such that (CtPn)An(C_{t}\cap P_{n})\setminus A_{n}\neq\emptyset for all λ\lambda-tableaux tt, then λΩ2(n)\lambda\notin\Omega_{2}(n).

Proof.

By Lemma 2.3, it is sufficient to prove that πPnetπ=0\sum_{\pi\in P_{n}}e_{t}\pi=0 for all λ\lambda-tableaux tt. Let tt be a λ\lambda-tableau, and let τCtPn\tau\in C_{t}\cap P_{n} such that sign(τ)=1sign(\tau)=-1. Then we have:

πPnetπ=πPnσCtsign(σ){t}σπ=πPnσCtsign(σ){t}σ(τπ)=\sum_{\pi\in P_{n}}e_{t}\pi=\sum_{\pi\in P_{n}}\sum_{\sigma\in C_{t}}sign(\sigma)\{t\}\sigma\pi=\sum_{\pi\in P_{n}}\sum_{\sigma\in C_{t}}sign(\sigma)\{t\}\sigma(\tau\pi)=
=πPnσCtsign(σ){t}(στ)π=πPnσCtsign(σ){t}σπ=πPnetπ.=\sum_{\pi\in P_{n}}\sum_{\sigma\in C_{t}}sign(\sigma)\{t\}(\sigma\tau)\pi=-\sum_{\pi\in P_{n}}\sum_{\sigma\in C_{t}}sign(\sigma)\{t\}\sigma\pi=-\sum_{\pi\in P_{n}}e_{t}\pi.

Proposition 2.6.

Let n>0n>0 be an integer. If λΩ2(n)\lambda\in\Omega_{2}(n) then λ\lambda has at most n2\lceil\frac{n}{2}\rceil parts.

Proof.

Let λΩ2(n)\lambda\in\Omega_{2}(n). We know that (2k+1,2k+2)Pn(2k+1,2k+2)\in P_{n} for all kk such that 22k+2n2\leq 2k+2\leq n. By Lemma 2.5, there must be a λ\lambda-tableau tt such that none of these 22-cycles lies in CtC_{t}. In particular, if either of the elements {2k+1,2k+2}\{2k+1,2k+2\} lies in the first column of tt, then the other must be in another. This means that the first column of [λ][\lambda] can have at most n2\lceil\frac{n}{2}\rceil boxes. ∎

This is in fact an exact bound, since by Proposition 2.4 we know that (2n)=(2,, 2)Ω2(2n)(2^{n})=(2,\ldots,\,2)\in\Omega_{2}(2n), and Proposition 2.8 will also yield (2n, 1)Ω2(2n+1)(2^{n},\,1)\in\Omega_{2}(2n+1).
We will now prove two useful conditions for constructing Ω2(n)\Omega_{2}(n) inductively. These are essentially a slight modification to the arguments used in [GL18] to reduce the odd prime case. The first proposition allows us to construct some of the partitions in Ω2(2k+1)\Omega_{2}(2^{k+1}) from partitions in Ω2(2k)\Omega_{2}(2^{k}).

Proposition 2.7.

Let k>0k>0 be an integer. Let μ,νΩ2(2k)\mu,\nu\in\Omega_{2}(2^{k}) such that μν\mu\neq\nu. If λ𝒫(2k+1)\lambda\in\mathcal{P}(2^{k+1}) is such that [χλ,(χμ×χν)S2k+1]0[\chi^{\lambda},\,(\chi^{\mu}\times\chi^{\nu})\uparrow^{S_{2^{k+1}}}]\neq 0, then λΩ2(2k+1)\lambda\in\Omega_{2}(2^{k+1}).

Proof.

Suppose λ𝒫(2k+1)\lambda\in\mathcal{P}(2^{k+1}) and μ,νΩ2(2k)\mu,\nu\in\Omega_{2}(2^{k}) are as stated above. We have a natural embedding S2k×S2kS2kC2S2k+1S_{2^{k}}\times S_{2^{k}}\trianglelefteq S_{2^{k}}\wr C_{2}\leq S_{2^{k+1}} (where the first is a Young subgroup and C2C_{2} acts on it by swapping the elements the copies of S2kS_{2^{k}} act on). Then P2k×P2kSyl2(S2k×S2k)P_{2^{k}}\times P_{2^{k}}\in\mathrm{Syl}_{2}(S_{2^{k}}\times S_{2^{k}}) and P2kC2Syl2(S2k+1)P_{2^{k}}\wr C_{2}\in\mathrm{Syl}_{2}(S_{2^{k+1}}). Since S2k×S2kS2kC2S_{2^{k}}\times S_{2^{k}}\trianglelefteq S_{2^{k}}\wr C_{2} we can apply Clifford Theory to χμ×χν\chi^{\mu}\times\chi^{\nu}. The inertial subgroup of this character is S2k×S2kS_{2^{k}}\times S_{2^{k}} (since μν\mu\neq\nu), so (χμ×χν)S2kC2(\chi^{\mu}\times\chi^{\nu})\uparrow^{S_{2^{k}}\wr C_{2}} is irreducible. This means that (χμ×χν)S2kC2(\chi^{\mu}\times\chi^{\nu})\uparrow^{S_{2^{k}}\wr C_{2}} is an irreducible constituent of χλS2kC2\chi^{\lambda}\downarrow_{S_{2^{k}}\wr C_{2}}. Since (S2k×S2k)(P2kC2)=P2k×P2k(S_{2^{k}}\times S_{2^{k}})\cap(P_{2^{k}}\wr C_{2})=P_{2^{k}}\times P_{2^{k}} and (S2k×S2k)(P2kC2)=S2kC2(S_{2^{k}}\times S_{2^{k}})\cdot(P_{2^{k}}\wr C_{2})=S_{2^{k}}\wr C_{2}, we have that:

[(χμ×χν)S2kC2P2kC2, 1P2kC2]=[(χμ×χν)P2k×P2kP2kC2, 1P2kC2]=[(\chi^{\mu}\times\chi^{\nu})\uparrow^{S_{2^{k}}\wr C_{2}}\downarrow_{P_{2^{k}}\wr C_{2}},\,1_{P_{2^{k}}\wr C_{2}}]=[(\chi^{\mu}\times\chi^{\nu})\downarrow_{P_{2^{k}}\times P_{2^{k}}}\uparrow^{P_{2^{k}}\wr C_{2}},\,1_{P_{2^{k}}\wr C_{2}}]=
=[(χμ×χν)P2k×P2k, 1P2k×P2k]0=[(\chi^{\mu}\times\chi^{\nu})\downarrow_{P_{2^{k}}\times P_{2^{k}}},\,1_{P_{2^{k}}\times P_{2^{k}}}]\neq 0

since μ,νΩ2(2k)\mu,\nu\in\Omega_{2}(2^{k}). ∎

The second proposition allows us to construct the elements of Ω2(n)\Omega_{2}(n) starting from Ω2(2k)\Omega_{2}(2^{k}).

Proposition 2.8.

Let n>0n>0 be an integer. Write n=i=1t2ain=\sum_{i=1}^{t}2^{a_{i}} with aia_{i} distinct (here we do not require any specific ordering). Let 1j<t1\leq j<t and m=i=1j2aim=\sum_{i=1}^{j}2^{a_{i}}. Let λ𝒫(n)\lambda\in\mathcal{P}(n). Then λΩ2(n)\lambda\in\Omega_{2}(n) if and only if there exist μΩ2(m)\mu\in\Omega_{2}(m) and νΩ2(nm)\nu\in\Omega_{2}(n-m) such that [χλ,(χμ×χν)Sn]0[\chi^{\lambda},\,(\chi^{\mu}\times\chi^{\nu})\uparrow^{S_{n}}]\neq 0.

Proof.

Consider the following subgroups Pm×PnmSm×SnmSnP_{m}\times P_{n-m}\leq S_{m}\times S_{n-m}\leq S_{n}. Pm×PnmP_{m}\times P_{n-m} is a Sylow 22-subgroup of SnS_{n}. This means that [χλPm×Pnm, 1Pm×Pnm]0[\chi^{\lambda}\downarrow_{P_{m}\times P_{n-m}},\,1_{P_{m}\times P_{n-m}}]\neq 0 if and only if χλSm×Snm\chi^{\lambda}\downarrow_{S_{m}\times S_{n-m}} has an irreducible constituent whose restriction to Pm×PnmP_{m}\times P_{n-m} satisfies the same condition. The irreducible characters of Sm×SnmS_{m}\times S_{n-m} satisfying this condition are exactly those of the form χμ×χν\chi^{\mu}\times\chi^{\nu} where μΩ2(m)\mu\in\Omega_{2}(m) and νΩ2(nm)\nu\in\Omega_{2}(n-m). ∎

Let’s use this proposition to determine the sets Ω2(n)(n)\Omega_{2}(n)\cap\mathcal{H}(n) and Ω2(n)𝒜(n)\Omega_{2}(n)\cap\mathcal{AH}(n). In both cases we choose to parametrize these sets using the number of parts of the partitions.

Lemma 2.9.

Let nn be a positive integer and n=2a1+2a2++2atn=2^{a_{1}}+2^{a_{2}}+\cdots+2^{a_{t}} its binary expansion. We have that (n(l1), 1l1)Ω2(n)(n)(n-(l-1),\,1^{l-1})\in\Omega_{2}(n)\cap\mathcal{H}(n) if and only if ltl\leq t.

Proof.

We prove the result by induction on the number of elements in the binary expansion of nn. If nn is a power of 22 the result follows from [Gia17, Theorem 1.1]. Let n=2a1+2a2++2atn=2^{a_{1}}+2^{a_{2}}+\cdots+2^{a_{t}} with t2t\geq 2. Let N=2a1++2at1N=2^{a_{1}}+\cdots+2^{a_{t-1}}. By Proposition 2.8 and the Littlewood-Richardson Rule, λΩ2(n)\lambda\in\Omega_{2}(n) if and only if there exist μΩ2(N)\mu\in\Omega_{2}(N) and νΩ2(2at)\nu\in\Omega_{2}(2^{a_{t}}) that are both subpartitions of λ\lambda and such that [λμ][\lambda\setminus\mu] has a L-R filling of weight ν\nu. If λ(n)\lambda\in\mathcal{H}(n) we must have μ(N)\mu\in\mathcal{H}(N) and ν(2at)\nu\in\mathcal{H}(2^{a_{t}}). Therefore, μ=(N(l11), 1l11)\mu=(N-(l_{1}-1),\,1^{l_{1}-1}) with l1t1l_{1}\leq t-1 and ν\nu is the trivial partition. This implies that λ\lambda has at most tt parts. Vice versa, if λ=(n(l1), 1l1)\lambda=(n-(l-1),\,1^{l-1}) with 2lt2\leq l\leq t (the trivial partition is clearly in Ω2(n)\Omega_{2}(n)), then we consider μ=(N(l2), 1l2)\mu=(N-(l-2),\,1^{l-2}) and the L-R filling consisting of filling each box with the number 11. ∎

Let us observe here that, in the case n=2kn=2^{k} we have Ω2(2k)(2k)={(2k)}\Omega_{2}(2^{k})\cap\mathcal{H}(2^{k})=\{(2^{k})\}. This fact will be used in subsequent proofs without being explicitly recalled.

Lemma 2.10.

Let n4n\geq 4 be a positive integer and n=2a1+2a2++2atn=2^{a_{1}}+2^{a_{2}}+\cdots+2^{a_{t}} its binary expansion, with a1>>ata_{1}>\cdots>a_{t}. We have that (nl, 2, 1l2)Ω2(n)𝒜(n)(n-l,\,2,\,1^{l-2})\in\Omega_{2}(n)\cap\mathcal{AH}(n) if and only if la1+t1l\leq a_{1}+t-1.

Proof.

We proceed by induction, as in the previous lemma. The base case is given by [GuL25, Theorem 1.3]. Let n=2a1+2a2++2atn=2^{a_{1}}+2^{a_{2}}+\cdots+2^{a_{t}} with t2t\geq 2. Let N=2a1++2at1N=2^{a_{1}}+\cdots+2^{a_{t-1}}. By Proposition 2.8 and the L-R Rule, λΩ2(n)\lambda\in\Omega_{2}(n) if and only if there exist μΩ2(N)\mu\in\Omega_{2}(N) and νΩ2(2at)\nu\in\Omega_{2}(2^{a_{t}}) that are both subpartitions of λ\lambda and such that [λμ][\lambda\setminus\mu] has a Littlewood-Richardson filling of weight ν\nu. If λ𝒜(n)\lambda\in\mathcal{AH}(n) we must have μ𝒜(N)(N)\mu\in\mathcal{AH}(N)\cup\mathcal{H}(N) and ν𝒜(2at)(2at)\nu\in\mathcal{AH}(2^{a_{t}})\cup\mathcal{H}(2^{a_{t}}). Also, at least one of the two must be a hook partition: if μ𝒜(N)\mu\in\mathcal{AH}(N), then any L-R filling of [λμ][\lambda\setminus\mu] has weight a hook partition. If ν(2at)Ω2(2at)\nu\in\mathcal{H}(2^{a_{t}})\cap\Omega_{2}(2^{a_{t}}), then it must be the trivial partition. At the same time, μ\mu has at most a1+t2a_{1}+t-2 parts, so λ\lambda has at most a1+t1a_{1}+t-1. If ν𝒜(2at)Ω2(2at)\nu\in\mathcal{AH}(2^{a_{t}})\cap\Omega_{2}(2^{a_{t}}) (which implies at2a_{t}\geq 2, otherwise there are no almost-hook partitions), then ν\nu has at most ata_{t} parts. In this case μ(N)Ω2(n)\mu\in\mathcal{H}(N)\cap\Omega_{2}(n), so μ\mu has at most t1t-1 parts. Therefore, λ\lambda has at most at+t1a1+t1a_{t}+t-1\leq a_{1}+t-1 parts. Vice versa, if λ=(nl, 2, 1l2)\lambda=(n-l,\,2,\,1^{l-2}) with 3la1+t13\leq l\leq a_{1}+t-1, then take μ=(N(l1), 2, 1l3)\mu=(N-(l-1),\,2,\,1^{l-3}) and the Littlewood-Richardson filling of [λμ][\lambda\setminus\mu] obtained by filling each box with 11. The partition (n2, 2)(n-2,\,2) is in Ω2(n)\Omega_{2}(n), by Proposition 2.4 and the L-R Rule when nn is odd. ∎

This second result shows the maximality of the bound that we will prove in Theorem 4.3.

3. The power of 2 case

To simplify notation we will define the following sets of partitions.

Definition 3.1.

Let nn and kk be positive integers. We let Δ(n,k)\Delta(n,k) be the subset of 𝒫(n)(n)\mathcal{P}(n)\setminus\mathcal{H}(n) of partitions with at most kk parts.

We will proceed in the natural way suggested by the structure of the Sylow 22-subgroups of SnS_{n} and by Propositions 2.7 and 2.8: in this section we will prove the desired result for powers of 22, and then generalize to all positive integers in the next. For the first step we will use the two following lemmas.

Lemma 3.2.

Let n4n\geq 4 be an integer; then

Δ(2n,4)Ω2(2n).\Delta(2^{n},4)\subseteq\Omega_{2}(2^{n}).
Proof.

We prove this lemma by induction. The base case n=4n=4 has been checked using [GAP]. Let n>4n>4 and λΔ(2n,4)\lambda\in\Delta(2^{n},4). We will prove that λΩ2(2n)\lambda\in\Omega_{2}(2^{n}) by using Proposition 2.7 and the Littlewood-Richardson Rule: it is sufficient to find a subpartition μΔ(2n1,4)\mu\in\Delta(2^{n-1},4) of λ\lambda and a L-R filling of [λμ][\lambda\setminus\mu] of weight νΔ(2n1,4){(2n1)}\nu\in\Delta(2^{n-1},4)\cup\{(2^{n-1})\}, such that μν\mu\neq\nu.
Consider the following algorithm: mark the first 2n12^{n-1} boxes of [λ][\lambda] going from top to bottom, from left to right. The marked boxes form the Young diagram of a subpartition μ𝒫(2n1)\mu\in\mathcal{P}(2^{n-1}) of λ\lambda. Furthermore, since λ(2n)\lambda\notin\mathcal{H}(2^{n}), we have that μ(2n1)\mu\notin\mathcal{H}(2^{n-1}) (box (2, 2)(2,\,2) is necessarily marked); therefore μΔ(2n1,4)\mu\in\Delta(2^{n-1},4), as desired. We then fill [λμ][\lambda\setminus\mu] with the L-R filling described in Remark 2.2 and call it’s weight ν𝒫(2n1)\nu\in\mathcal{P}(2^{n-1}). If νΔ(2n1,4){(2n1)}\nu\in\Delta(2^{n-1},4)\cup\{(2^{n-1})\} and μν\mu\neq\nu, then we have obtained the desired result.
Let’s suppose that μ=ν\mu=\nu. This implies that ν1=μ1=λ1\nu^{\prime}_{1}=\mu^{\prime}_{1}=\lambda^{\prime}_{1}, which means that all columns of [μ][\mu], except possibly the last, must have λ1\lambda^{\prime}_{1} boxes. If λ1=1, 2, 4\lambda^{\prime}_{1}=1,\,2,\,4 then, since λ1\lambda^{\prime}_{1} divides 2n12^{n-1} and μ=ν\mu=\nu, we have that:

λ{(2n),(2n1, 2n1),(2n2, 2n2, 2n2, 2n2)}Ω2(2n)\lambda\in\{(2^{n}),\,(2^{n-1},\,2^{n-1}),\,(2^{n-2},\,2^{n-2},\,2^{n-2},\,2^{n-2})\}\subseteq\Omega_{2}(2^{n})

(by Proposition 2.4). Suppose λ1=3\lambda^{\prime}_{1}=3; if the last column of [μ][\mu] is made of two cells, then [ν][\nu] has a column with just one cell; if the last column of [μ][\mu] has one cell, then [ν][\nu] has a column with two cells. This means that if λ1=3\lambda^{\prime}_{1}=3 then μν\mu\neq\nu.
Suppose ν\nu is a non-trivial hook partition. For this to occur, [λμ][\lambda\setminus\mu] must have a single column with more than one box. Every column of [λμ][\lambda\setminus\mu] from the second onward contains all the corresponding boxes in the respective column of [λ][\lambda], due to how the algorithm is defined. For this reason, the column of [λμ][\lambda\setminus\mu] with more than one box must be the first or the second.
If the column is the first, we modify the output of the algorithm by marking the last unmarked box in this column, and unmarking the last box of the previous one. We maintain the same filling for all previously unmarked boxes, and input the number 22 in the newly unmarked one. This is a L-R filling. This gives us two new partitions μ0\mu^{0} and ν0\nu^{0}. Now [μ0][\mu^{0}] has at least 55 columns of which all but the last two have at least 22 boxes. Meanwhile, [ν0][\nu^{0}] has exactly two columns with more than one box. This means that both partitions are non hook partitions, and they are distinct.
If instead the column of [λμ][\lambda\setminus\mu] is the second one, then we just replace the 11 in the first column with a 22, and conclude as before. ∎

The next lemma will allow us to increase the number of parts as we increase nn.

Lemma 3.3.

Let nk4n\geq k\geq 4 be integers such that Δ(2n,k)Ω2(2n)\Delta(2^{n},k)\subseteq\Omega_{2}(2^{n}) and Δ(2n+1,k)Ω2(2n+1)\Delta(2^{n+1},k)\subseteq\Omega_{2}(2^{n+1}); then we have that

Δ(2n+1,k+1)Ω2(2n+1).\Delta(2^{n+1},k+1)\subseteq\Omega_{2}(2^{n+1}).
Proof.

Suppose that nn and kk satisfy the above conditions. Let λΔ(2n+1,k+1)Δ(2n+1,k)\lambda\in\Delta(2^{n+1},k+1)\setminus\Delta(2^{n+1},k). We will prove that λΩ2(2n+1)\lambda\in\Omega_{2}(2^{n+1}), as in Lemma 3.2, by using Proposition 2.7 and the Littlewood-Richardson Rule. We will construct two partitions μ,νΔ(2n,k){(2n)}Ω2(2n)\mu,\nu\in\Delta(2^{n},k)\cup\{(2^{n})\}\subseteq\Omega_{2}(2^{n}) such that μν\mu\neq\nu and there is a L-R filling of [λμ][\lambda\setminus\mu] of weight ν\nu. Consider the following algorithm on [λ][\lambda]: mark the first kk boxes of the first column, the first two of the second, and then continue marking from left to right, top to bottom until the marked cells form the Young diagram of a partition μΔ(2n,k)\mu\in\Delta(2^{n},k). Note that μ\mu cannot have k+1k+1 parts, because this would require marking more than 2n2^{n} boxes (we will omit similar observations in other subsequent proofs). Then fill the boxes of [λμ][\lambda\setminus\mu] as in Remark 2.2 and let ν𝒫(2n)\nu\in\mathcal{P}(2^{n}) be its weight.
Firstly, let us prove that ν\nu has at most kk parts. To do this, we will prove this slightly stronger fact: in applying the algorithm, we mark at least one cell in every column of [λ][\lambda] with at least kk cells. Suppose that λ\lambda is such that this doesn’t happen. Let tt be the index of the first untouched column (which must have at least kk elements). Since k+2n+2<2nk+2\leq n+2<2^{n}, tt must be at least 44. The number of marked boxes is k+2+t3=2nk+2+t-3=2^{n}. The number of unmarked boxes in the first tt columns is at least 1+k2+(k1)(t3)+k1+k-2+(k-1)(t-3)+k, and it must not exceed 2n2^{n} (the total number of unmarked boxes). This gives the following inequality:

1+k2+(k1)(t3)+kk+2+t31+k-2+(k-1)(t-3)+k\leq k+2+t-3
3(k2)(t3)+k30.3\leq(k-2)(t-3)+k-3\leq 0.

The reason why we proved this stronger result is that this can also be used to prove that μν\mu\neq\nu. Suppose that μ\mu and ν\nu have the same number of parts. By the previous observation there must be at least one column of [λ][\lambda] with k+1k+1 boxes of which only one is marked. Due to how the algorithm is defined, this column can’t be the first nor the second. Therefore the second column of [λ][\lambda] is made of k+1k+1 boxes, of which only two are marked (the third can’t be marked, otherwise all boxes in the second row would also be marked). This means that [μ][\mu] has one column with kk boxes, and all others with two or less. Meanwhile, ν\nu has a column with (k+1)2=k13(k+1)-2=k-1\geq 3 boxes, and therefore μν\mu\neq\nu. This leaves the case in which ν\nu is a non-trivial hook partition.
Suppose that ν\nu is a non-trivial hook partition. By the previous observation, ν\nu cannot have kk parts. This means that if we modify the partitions μ\mu and ν\nu without changing the number of their parts, then they will still be distinct. Just as in the proof of Lemma 3.2, if ν\nu is a hook partition, then [λμ][\lambda\setminus\mu] has only one column with more than one box. If the other boxes of [λμ][\lambda\setminus\mu] are not all in the same row, it suffices to change the content of the last box of the last of these rows (excluding all elements of the column with more than one box) from a 11 to a 22. This changes ν\nu into a non hook partition, without modifiying the number of parts.
The last remaining case is that in which all the cells of [λμ][\lambda\setminus\mu] lie in the union of a column and a row. This is impossible. If this were to happen, this would mean that the row considered is the (k+1)(k+1)-th, since the last box of the first column of [λ][\lambda] is left unmarked. Therefore, the number of cells in [λμ][\lambda\setminus\mu] is at most λk+1+k1\lambda_{k+1}+k-1, while the number of marked cells is at least k(λk+11)k(\lambda_{k+1}-1); this results in the inequality λk+1+k1k(λk+11)\lambda_{k+1}+k-1\geq k(\lambda_{k+1}-1), which isn’t satisfiable for k4k\geq 4 and λk+12n(k1)13\lambda_{k+1}\geq 2^{n}-(k-1)\geq 13. ∎

We will now give an example of the algorithm described in Lemma 3.3.

Example 3.4.

Let λ=(25, 23, 1)Δ(32,5)Δ(32,4)\lambda=(25,\,2^{3},\,1)\in\Delta(32,5)\setminus\Delta(32,4). The algorithm gives us the following figure

    ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   11   11   11   11   11   11   11   11   11   11   11   11   11        ×\times   ×\times        ×\times   11        ×\times   22        11   

The output is μ=(12, 2, 12)\mu=(12,\,2,\,1^{2}) e ν=(15, 1)\nu=(15,\,1). We have ν(16){(16)}\nu\in\mathcal{H}(16)\setminus\{(16)\} so we must apply the modification described in Lemma 3.3.

    ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   ×\times   11   11   11   11   11   11   11   11   11   11   11   11   11        ×\times   ×\times        ×\times   11        ×\times   22        22   

Now μ=(12, 2, 12)\mu=(12,\,2,\,1^{2}) e ν=(14, 2)\nu=(14,\,2).

The proof of the desired bound in the case of powers of 22 is now essentially complete.

Proposition 3.5.

Let n4n\geq 4 be an integer. Then

Δ(2n,n)Ω2(2n).\Delta(2^{n},n)\subseteq\Omega_{2}(2^{n}).
Proof.

We will prove by induction on n4n\geq 4 that for all mnm\geq n, we have Δ(2m,n)Ω2(2m)\Delta(2^{m},n)\subseteq\Omega_{2}(2^{m}), which is equivalent to the statement above. The base case is given by Lemma 3.2. Let n>4n>4 such that for all Nn1N\geq n-1, we have Δ(2N,n1)Ω2(2N)\Delta(2^{N},n-1)\subseteq\Omega_{2}(2^{N}). Let mnm\geq n, then m,m1n14m,\,m-1\geq n-1\geq 4, so Δ(2m1,n1)Ω2(2m1)\Delta(2^{m-1},n-1)\subseteq\Omega_{2}(2^{m-1}) and Δ(2m,n1)Ω2(2m)\Delta(2^{m},n-1)\subseteq\Omega_{2}(2^{m}). By Lemma 3.3 we have Δ(2m,n)Ω2(2m)\Delta(2^{m},n)\subseteq\Omega_{2}(2^{m}). ∎

To prove the corresponding result for all positive integers we will require a slightly stronger bound for powers of 22, obtained by excluding almost-hook partitions. This we present as the following proposition.

Proposition 3.6.

If n4n\geq 4 is an integer, then

Δ(2n,2n3)𝒜(2n)Ω2(2n).\Delta(2^{n},2n-3)\setminus\mathcal{AH}(2^{n})\subseteq\Omega_{2}(2^{n}).
Proof.

We prove this result by induction on n4n\geq 4. The base case has been checked with [GAP]. Let n>4n>4, such that the statement is true for n1n-1. Let λΔ(2n,2n3)(Δ(2n,n)𝒜(2n))\lambda\in\Delta(2^{n},2n-3)\setminus(\Delta(2^{n},n)\cup\mathcal{AH}(2^{n})). Let 1kn31\leq k\leq n-3 be the integer such that n+kn+k is the number of parts of λ\lambda. Just as in Lemma 3.3, we will provide an algorithm that gives two partitions μ,νΩ2(2n1)\mu,\nu\in\Omega_{2}(2^{n-1}), such that μν\mu\neq\nu and there is a L-R filling of [λμ][\lambda\setminus\mu] of weight ν\nu. The algorithm is the following: mark the first n1n-1 cells in the first column of [λ][\lambda], then the first max{2,λ2(n2)}\mathrm{max}\{2,\,\lambda_{2}^{\prime}-(n-2)\} in the second, then the first max{1,λi(n1)}\mathrm{max}\{1,\,\lambda_{i}^{\prime}-(n-1)\} in the ii-th column (starting from i=3i=3), until 2n12^{n-1} cells have been marked or the last column has been reached. If the number of marked cells is less than 2n12^{n-1}, we reach that number by marking boxes from left to right, top to bottom (we will refer to this phase as the filling phase). As before, we call the partition corresponding to the obtained diagram μ\mu, while ν\nu is the partition obtained as the weight of the usual filling of [λμ][\lambda\setminus\mu] (Remark 2.2). Clearly μΔ(2n1,n1)\mu\in\Delta(2^{n-1},n-1).
Firstly, we will prove that ν\nu has at most n1n-1 parts. To do this we will prove a stronger fact which will be used later: the algorithm can’t terminate before marking all the required cells in each of the columns with at least n1n-1 boxes, plus one more. If the algorithm were to terminate by marking max{1,λi(n1)}\mathrm{max}\{1,\,\lambda_{i}^{\prime}-(n-1)\} or less boxes in a column with n1n-1 boxes or more, this would mean that, since each column has at most 2n32n-3 boxes, the number of marked cells in each column is at most n1n-1. Let ll be the number of columns of [λ][\lambda] with at least n1n-1 cells. The number of marked cells must be 2n12^{n-1}, therefore we must have:

l2n1n1.l\geq\frac{2^{n-1}}{n-1}.

Note that, since the filling phase isn’t necessary in this case, in each column with at least n1n-1 elements from the third onward the number of marked cells is strictly smaller than the number of unmarked cells. Let’s call the number of marked cells in these columns tt: the number of unmarked cells in these columns is at least t+l2t+l-2. Let mm be the number of marked cells in the first ll columns and uu the number of unmarked cells in these same columns:

(n1)+(k+2)+tm=2n1u(k+1)+(n3)+t+l2(n-1)+(k+2)+t\geq m=2^{n-1}\geq u\geq(k+1)+(n-3)+t+l-2
5l2n1n1.5\geq l\geq\frac{2^{n-1}}{n-1}.

This is possible only when n=5n=5. If n=5n=5, there are only five partitions of 1616 whose diagrams have at most 44 rows and 55 columns: the conjugate partitions of (44)(4^{4}), (43, 3, 1)(4^{3},\,3,\,1), (43, 22)(4^{3},\,2^{2}), (42, 32, 2)(4^{2},\,3^{2},\,2) e (4, 34)(4,\,3^{4}). In this case 2n3=72n-3=7 so [λ][\lambda] has at most 77 cells in each column. In the situation above, the algorithm marks at most 33 cells in each column after the second: therefore, μ\mu^{\prime} can’t be any of the first three. If μ\mu^{\prime} were one of the other two partitions, then μ3=3\mu_{3}^{\prime}=3, which means that λ3=7\lambda_{3}^{\prime}=7, so λ2=7\lambda_{2}^{\prime}=7 and μ2=4\mu_{2}^{\prime}=4. This leaves (42, 32, 2)(4^{2},\,3^{2},\,2). In this case λ=(74, 6,)\lambda^{\prime}=(7^{4},\,6,\,\ldots), which isn’t a partition of 3232. This proves that ν\nu has at most n1n-1 parts.
Suppose μ=ν\mu=\nu. This means that there is a column in [λ][\lambda] that comes after the second and has n+in+i boxes, with i0i\geq 0, of which exactly i+1i+1 have been marked. We deduce from this that no boxes were marked in the (i+3)(i+3)-th column during the
filling phase of the algorithm. The second column is λ2=n+j\lambda_{2}^{\prime}=n+j with jij\geq i. Since j+2i+2j+2\geq i+2, exactly j+2j+2 boxes have been marked in the second column. Therefore, [μ][\mu] has one column with n1n-1 boxes, and all others with at most j+2j+2; meanwhile, ν\nu has at least one column with n1n-1 boxes and at least one with n2n-2. If n2>j+2n-2>j+2, then μν\mu\neq\nu. This leaves j=n4,n3j=n-4,n-3. In these cases, unmark the last cell marked and mark the first unmarked cell in the first column of [λ][\lambda]. We replace μ\mu with the partition corresponding to the new diagram made of marked boxes. We then fill [λμ][\lambda\setminus\mu] using the same rule as before. The new partitions μ\mu and ν\nu are now such that μ\mu has n1+12(n1)3n-1+1\leq 2(n-1)-3 parts, and a column with j+2n23j+2\geq n-2\geq 3 boxes, so μΩ2(2n1)\mu\in\Omega_{2}(2^{n-1}) since it isn’t a hook or almost-hook partition. Meanwhile, ν\nu has n1n-1 parts and a column with n23n-2\geq 3 boxes, so it isn’t a hook partition.
The remaining case is that in which ν\nu is a non trivial hook partition. By the proof above, we know that, in this case, ν\nu has at most n2n-2 parts. Just as in Lemma 3.3 we can suppose that the unmarked cells lie in the union of a column and a row of [λ][\lambda] (otherwise we can change a 11 to a 22 in the filling). The column must be the first: we know that the boxes in the nn-th and n+1n+1-th positions of this column are left unmarked. The row must be the first. If this weren’t true, let ll be the number of unmarked elements in this row that aren’t in the first column. Counting marked and unmarked boxes, we have l+(n2)l+(n1)l+(n-2)\geq l+(n-1). Therefore the algorithm has terminated before the
filling phase, marking all boxes of the columns from the second onward until it stops before a column with just one part. This can only happen if λ(2n)𝒜(2n)\lambda\in\mathcal{H}(2^{n})\cup\mathcal{AH}(2^{n}).

4. The general case

The first step towards generalizing the bound we have now proven for powers of two will be to give a generalization of Proposition 3.6. This will yield most cases and, at the same time, give a useful instrument for handling the rest.

Proposition 4.1.

Let n16n\geq 16 be an integer. Suppose kk is the greatest integer such that 2kn2^{k}\leq n. Then

Δ(n,2k3)𝒜(n)Ω2(n).\Delta(n,2k-3)\setminus\mathcal{AH}(n)\subseteq\Omega_{2}(n).
Proof.

Suppose nn and kk satisfy the conditions above, and λΔ(n,2k3)𝒜(n)\lambda\in\Delta(n,2k-3)\setminus\mathcal{AH}(n). We can assume that nn is even: if nn is odd, just remove any box of [λ][\lambda] such that the remaining diagram doesn’t correspond to a hook or almost-hook partition. We will use the Littlewood-Richardson Rule and Proposition 2.8 to reduce to the base case proven in Proposition 3.6. We will do so by finding μΔ(2k,2k3)𝒜(2k)\mu\in\Delta(2^{k},2k-3)\setminus\mathcal{AH}(2^{k}) a subpartition of λ\lambda, and a L-R filling of [λμ][\lambda\setminus\mu] of weight ν\nu, a partition with all parts even (Proposition 2.4).
We define the following algorithm: consider the last box in each column of [λ][\lambda], going from right to left, mark the maximum even number of these, such that the remaining boxes form the diagram of a partition which is not a hook nor an almost-hook partition. Remove the marked boxes of [λ][\lambda] and the columns in which no boxes have been marked. Repeat on the new diagram. Interrupt the algorithm once exactly n2kn-2^{k} boxes have been marked or the diagram that’s left is empty. Let μ\mu be the subpartition of λ\lambda corresponding to the diagram made up of all the unmarked cells in [λ][\lambda]. Then use the usual L-R filling (Remark 2.2) of [λμ][\lambda\setminus\mu]: it’s weight is clearly a partition with all parts even (ν1\nu_{1} is the number of cells marked at the first iteration, ν2\nu_{2} the number marked at the second, and so on). All that’s left to prove is that it is, in fact, a partition of n2kn-2^{k}. To do this, we will show that the algorithm cannot terminate before marking that many boxes. Suppose that the algorithm ends without marking n2kn-2^{k} boxes (so it reaches an empty set of boxes). Due to the algorithm’s definition there can’t be more than 2k32k-3 unmarked boxes in the first column, 2k42k-4 in the second, 2k52k-5 in the third, and so on. This is clear when the algorithm operates
smoothly, by which we mean that we can always mark the maximal number of boxes without leaving a hook or almost-hook partition. If at some iteration the algorithm cannot remove a box from the second column because this would make the remaining diagram an almost-hook partition, this means that there are only three boxes left in the second column and at most two in the ones following it. One box in the fourth column is marked at this iteration. The algorithm resumes its function regularly from the third or fourth column, which means that there are at most 33 unmarked boxes in the second column, 22 in the third, and 11 in the fourth. If the algorithm cannot mark a cell in the third column, this means that there are only two unmarked cells in the second. Just as before we conclude that the number of unmarked boxes is at most 22 in the second, third, and fourth column, and 11 in the fifth. Therefore, the number of unmarked boxes can be at most (2k3)(2k2)2<2k\frac{(2k-3)(2k-2)}{2}<2^{k}, so the number of marked boxes must be greater than n2kn-2^{k} which gives a contradiction. ∎

The following example illustrates the functioning of the algorithm described in Proposition 4.1.

Example 4.2.

Let n=23=16+4+2+1n=23=16+4+2+1 and λ=(53, 42)\lambda=(5^{3},\,4^{2}). Then we can reduce to n=22n=22 by taking for example (53, 4, 3)(5^{3},\,4,\,3). We then apply the algorithm and obtain the following figure.

                  11           11   22           22         11   11   

In this case μ=(5, 4, 32, 1)\mu=(5,\,4,\,3^{2},\,1) and ν=(4, 2)\nu=(4,\,2).

For many nn, Proposition 4.1 gives a stronger result than the one we have set out to prove. In particular, let n=i=1t2ain=\sum_{i=1}^{t}2^{a_{i}}, with a1>>ata_{1}>\cdots>a_{t}, if a1+t12a13a_{1}+t-1\leq 2a_{1}-3, then Proposition 4.1 and Lemma 2.10 imply the desired result. There are, however, still an infinite number of cases that aren’t included in the above result (t{a11,a1,a1+1}t\in\{a_{1}-1,\,a_{1},\,a_{1}+1\}). These will be eliminated in the next and final proof of this paper.

Theorem 4.3.

Let nn be a positive integer. Let n=i=1t2ain=\sum_{i=1}^{t}2^{a_{i}}, with a1>>ata_{1}>\cdots>a_{t}. Let knk_{n} be the maximum integer such that Δ(n,kn)Ω2(n)\Delta(n,k_{n})\subseteq\Omega_{2}(n). Then:

kn={if n5 (formally, since 𝒫(n)(n)Ω2(n))1if n=6,8,102if n=9a1+t1if n=7 or n11k_{n}=\begin{cases}\infty&\mbox{if $n\leq 5$ (formally, since $\mathcal{P}(n)\setminus\mathcal{H}(n)\subseteq\Omega_{2}(n)$)}\\ 1&\mbox{if $n=6,8,10$}\\ 2&\mbox{if $n=9$}\\ a_{1}+t-1&\mbox{if $n=7$ or $n\geq 11$}\end{cases}
Proof.

All cases up to n=31n=31 have been verified using [GAP]. Let n32n\geq 32 and n=i=1t2ain=\sum_{i=1}^{t}2^{a_{i}} its binary decomposition, with a1>>ata_{1}>\cdots>a_{t}. Firstly, let us remind the reader that Lemma 2.10 provides the description of Ω2(n)𝒜(n)\Omega_{2}(n)\cap\mathcal{AH}(n), and at the same time proves kna1+t1k_{n}\leq a_{1}+t-1, so we just have to prove that Δ(n,a1+t1)𝒜(n)Ω2(n)\Delta(n,a_{1}+t-1)\setminus\mathcal{AH}(n)\subseteq\Omega_{2}(n). To do this we will use Proposition 2.8 and Proposition 4.1. Let λΔ(n,a1+t1)𝒜(n)\lambda\in\Delta(n,a_{1}+t-1)\setminus\mathcal{AH}(n). By Proposition 4.1 we may assume that a1+t12a12a_{1}+t-1\geq 2a_{1}-2 (which is to say t=a11,a1,a1+1t=a_{1}-1,\,a_{1},\,a_{1}+1) and that λ\lambda has at least 2a122a_{1}-2 parts. We will proceed by describing a similar algorithm on [λ][\lambda] to the one described in Proposition 4.1, such that the returned partitions μ𝒫(2a1)\mu\in\mathcal{P}(2^{a_{1}}) and ν𝒫(n2a1)\nu\in\mathcal{P}(n-2^{a_{1}}) are of the kinds whose behavior has been characterised in the various lemmas and propositions above. In particular we want to be able to apply Proposition 4.1 to μ\mu and ν\nu, so for this part of the proof we will assume n2a116n-2^{a_{1}}\geq 16 (equivalently a24a_{2}\geq 4).
The algorithm is the following: mark all boxes in the rows numbered 2a122a_{1}-2 onward; if the number of marked boxes hasn’t exceeded n2a1n-2^{a_{1}}, mark the last box of each column from right to left (if one of such boxes has already been marked, leave as is), then the second last, and so on until n2a1n-2^{a_{1}} cells have been marked. During the process, make sure to skip marking a box if the resulting diagram of unmarked boxes does not correspond to a partition or it corresponds to a hook or almost-hook partition. As before, we will call μ\mu the partition corresponding to the diagram made up of unmarked boxes, and ν\nu the partition obtained as the weight of the usual L-R filling of [λμ][\lambda\setminus\mu] (Remark 2.2). The first thing we must prove is that the algorithm always marks exactly n2a1n-2^{a_{1}} cells. The only way this may not occur is if λ2a12+λ2a11+λ2a1>n2a1\lambda_{2a_{1}-2}+\lambda_{2a_{1}-1}+\lambda_{2a_{1}}>n-2^{a_{1}}. If a16a_{1}\geq 6 some simple approximations show that this is impossible. To simplify notation, let s:=ta1+2s:=t-a_{1}+2 (the maximum number of parts following λ2a13\lambda_{2a_{1}-3}):

λ2a12+λ2a11+λ2a1n2a12s<2a1+12a12s\lambda_{2a_{1}-2}+\lambda_{2a_{1}-1}+\lambda_{2a_{1}}\leq\frac{n}{2a_{1}-2}\cdot s<\frac{2^{a_{1}+1}}{2a_{1}-2}\cdot s
n2a11++2a1+s4=2a1+s31n-2^{a_{1}}\geq 1+\cdots+2^{a_{1}+s-4}=2^{a_{1}+s-3}-1
182a12+12a1224s2a12s+12a1+s3.1\geq\frac{8}{2a_{1}-2}+\frac{1}{2^{a_{1}-2}}\geq\frac{2^{4-s}}{2a_{1}-2}\cdot s+\frac{1}{2^{a_{1}+s-3}}.

The inequality for the remaining cases (those with a1=5a_{1}=5 and a2=4a_{2}=4) has been checked with [GAP]. This means that μ\mu and ν\nu are partitions of the correct numbers. By the definition of the algorithm μΔ(2a1,2a13)𝒜(2a1)\mu\in\Delta(2^{a_{1}},2a_{1}-3)\setminus\mathcal{AH}(2^{a_{1}}).
Now we will prove that ν\nu has at most 2a232a_{2}-3 parts. If this weren’t true, we would have had to mark more than the set comprised of the last 2a232a_{2}-3 boxes in each column (except for the boxes (1,2)(1,2), (2,2)(2,2), (3,2)(3,2) or (1,2)(1,2), (2,2)(2,2), (1,3)(1,3), (2,3)(2,3)). The number of such boxes is at least λ1++λ2a234\lambda_{1}+\cdots+\lambda_{2a_{2}-3}-4. Therefore it suffices to prove that λ1++λ2a234n2a1\lambda_{1}+\cdots+\lambda_{2a_{2}-3}-4\geq n-2^{a_{1}} or equivalently that λ2a22++λa1+t1+42a1\lambda_{2a_{2}-2}+\cdots+\lambda_{a_{1}+t-1}+4\leq 2^{a_{1}}. As before, this is easy to prove for
large a1a_{1} (in this case a19a_{1}\geq 9), meanwhile, cases a1=6, 7, 8a_{1}=6,\,7,\,8 have been checked by hand using better approximations, and the case a1=5a_{1}=5 has been checked using [GAP]. For a19a_{1}\geq 9 the simple approximations used are the following (again s:=ta1+2s:=t-a_{1}+2):

a1+t12a2+32a1+s32(a14+s)+3=8sa_{1}+t-1-2a_{2}+3\leq 2a_{1}+s-3-2(a_{1}-4+s)+3=8-s
λ2a22++λa1+t1+4na1+t1(8s)+4<2a1+12a127+11\lambda_{2a_{2}-2}+\cdots+\lambda_{a_{1}+t-1}+4\leq\lceil\frac{n}{a_{1}+t-1}\rceil\cdot(8-s)+4<\frac{2^{a_{1}+1}}{2a_{1}-2}\cdot 7+11
142a12+112a11.\frac{14}{2a_{1}-2}+\frac{11}{2^{a_{1}}}\leq 1.

The only cases remaining now are those in which ν(n2a1)𝒜(n2a1)\nu\in\mathcal{H}(n-2^{a_{1}})\cup\mathcal{AH}(n-2^{a_{1}}). In this case we will prove that the number of parts of ν\nu is at most 3a12t13\leq a_{1}-2\leq t-1 so νΩ2(n2a1)\nu\in\Omega_{2}(n-2^{a_{1}}) (by Lemma 2.9 and Lemma 2.10). Suppose that ν\nu is a hook or almost-hook partition with at least four parts. This means that the algorithm has continued to the second phase, and has marked the last three cells in each column (excluding the ones of the type mentioned above). Since [ν][\nu] has at most two columns with more than one cell, only one of which (the first) has more than two cells, the first column of [ν][\nu] must correspond to the marked cells in the first column of [λ][\lambda], in which at least three boxes have been marked. At the third pass of the second phase of the algorithm, there must have been only one available cell to mark, and this must have been in the first column; this means that removing any other cell from the diagram gives an almost-hook partition or something that isn’t a partition. This means that μ\mu is of the form (m, 22)(m,\,2^{2})^{\prime} or (m, 3)(m,\,3)^{\prime} and in both cases m2a14m\leq 2a_{1}-4. However m+42a1<2a1m+4\leq 2a_{1}<2^{a_{1}} gives a contradiction.
There are now only a finite number of remaining cases: those n>32n>32 such that ta11t\geq a_{1}-1 and at the same time a2<4a_{2}<4. These numbers are 39, 43, 45, 46, 47, 7939,\,43,\,45,\,46,\,47,\,79. Each case can be solved by hand by reducing to a smaller nn. For example, let λ𝒫(39)\lambda\in\mathcal{P}(39) be a partition with 88 parts. Since 4<398<54<\frac{39}{8}<5, this means that λ15\lambda_{1}\geq 5 and λ84\lambda_{8}\leq 4. If λ8=1,2,4\lambda_{8}=1,2,4, let μ𝒫(38),𝒫(37),𝒫(35)\mu\in\mathcal{P}(38),\mathcal{P}(37),\mathcal{P}(35) (respectively) be the partition obtained by removing the last part, if λ8=3\lambda_{8}=3, let μ𝒫(35)\mu\in\mathcal{P}(35) be the partition corresponding to the diagram obtained from [λ][\lambda] by removing the last row and the last cell of the last column. In every case μ\mu is neither a hook nor almost-hook partition and the usual Littlewood-Richardson filling has weight corresponding to the trivial partition (of 1,21,2 or 44). We will omit the proof of the other cases, since they are very similar to the one above. ∎

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