#Plethysm
See [Hag07] and [LR10] for an introduction to calculations with plethysm. Another good reference is M. Zabrocki’s introduction to symmetric functions [Zab03, Ch. III].
#Representation-theoretic interpretation
Plethysm can easily be described using representation theory of \(\GL_n.\)
Let \(U,V,W\) be vector spaces over \(\setC,\) and consider polynomial representations \(\phi : \GL(U) \to \GL(V)\) and \(\psi : \GL(V) \to \GL(W).\) Let \(f\) and \(g\) be the corresponding characters (symmetric functions). The composition \(\psi\circ \phi : \GL(U) \to \GL(W)\) is then also a polynomial representation, and \(g[f]\) is the plethysm of \(g\) and \(f.\)
R. Orellana, F. Saliola, A. Schilling, and M. Zabrocki study plethysm through the uniform block permutation algebra, also called the party algebra [OSSZ22]. They define a Frobenius characteristic map whose character theory naturally produces plethysms of Schur functions.
This can be made more concrete, and extended to any symmetric function, see below.
#Definition
Plethysm is closely related to the power-sum symmetric functions. The following properties uniquely define plethysm, where \(f,\) \(g,\) and \(h\) denote symmetric functions with integer coefficients. Brackets are commonly used to denote plethystic substitutions.
\(\powerSum_k[\powerSum_m] = \powerSum_{km}.\)
\(\powerSum_k[f\pm g] = \powerSum_k[f] \pm \powerSum_k[g].\)
\(\powerSum_k[f\cdot g] = \powerSum_k[f] \cdot \powerSum_k[g].\)
\((f\pm g)[h] = f[h] \pm g[h].\)
\((f\cdot g)[h] = f[h] \cdot g[h].\)
Since every symmetric function can be expressed as a sum of products of \(\powerSum_k(\xvec),\) these properties uniquely determine the expression \(f[g].\)
The operator sending \(f(\xvec)\) to \(f(\xvec^k) = f[\powerSum_k(\xvec)]\) is called the \(k\)-th Adams operator. The adjoint to the Adams operator is the Verschiebung operator \(V_k,\) which is defined as \(V_k(\completeH_r) = \completeH_{r/k},\) if \(k \mid r,\) and \(0\) otherwise.
Example
Let us compute \(\powerSum_{22}[\powerSum_{43}]\): \[\begin{aligned} \powerSum_{22}[\powerSum_{43}] &= (\powerSum_{2}[\powerSum_{43}])^2 \\ &= (\powerSum_{2}[\powerSum_{4}] \cdot \powerSum_{2}[\powerSum_{3}])^2 \\ &= (\powerSum_{8} \cdot \powerSum_{6})^2 \\ &= \powerSum_{8866}. \end{aligned}\]
Similarly, \(\powerSum_{32}[3\powerSum_{4}]\) can be computed as \[\begin{aligned} \powerSum_{32}[3\powerSum_{4}] &= (\powerSum_{3}[\powerSum_{4}+\powerSum_{4}+\powerSum_{4}]) (\powerSum_{2}[\powerSum_{4}+\powerSum_{4}+\powerSum_{4}]) \\ &= (3\powerSum_{3}[\powerSum_{4}])(3\powerSum_{2}[\powerSum_{4}]) \\ &= 9\powerSum_{12} \cdot \powerSum_{8}. \end{aligned}\]
The situation is a bit more involved if the coefficients of \(f\) and \(g\) in the plethysm \(f[g]\) are formal power series in, say, \(\setC(\qvec).\)
We first define the plethysm \(\powerSum_k[g(\xvec)].\) If \(g(\xvec) = \sum_{\mu} d_\mu(\qvec) \powerSum_\mu(\xvec),\) then \[\powerSum_k[g(\xvec)] \coloneqq \sum_{\mu} d_\mu(q_1^k,q_2^k,\dotsc) \; \powerSum_{k\mu}(\xvec) .\] Let now \(f(\xvec) = \sum_{\lambda} c_\lambda(\qvec) \powerSum_\lambda(\xvec).\) Then \[f[g(\xvec)] \coloneqq \sum_{\lambda} c_\lambda(\qvec) \prod_{j=1}^{\length(\lambda)} \powerSum_{\lambda_j}[g(\xvec)].\] This definition agrees with the previous one in the case \(f\) and \(g\) are symmetric functions with integer coefficients, not depending on formal parameters.
Example
For example, \[\powerSum_{k}[5q \cdot \powerSum_{m}] = 5 q^k \powerSum_{km}.\]
Capital letters are sometimes used to denote the sum of the variables in that alphabet. For example, \(X = x_1+x_2+\dotsb = \elementaryE_1(\xvec).\)
A. D’Andrea, E. Fatighenti, and C. Onorati study a derivation \(\mathsf{D}\) on \(\spaceSym\) and prove a chain rule for \(\mathsf{D}\) with respect to plethysm [DFO25]. They also relate the Schur-support geometry of \(\mathsf{D}(f)\) to that of a homogeneous symmetric function \(f.\)
#Identities
We have the following identities:
\(\powerSum_{k}[qX] = q^k\powerSum_{k}[X]\)
\(\powerSum_{k}[-X] = -\powerSum_{k}[X]\)
\(\powerSum_{k}[\epsilon X] = \epsilon^k \powerSum_{k}[X]\) when \(\epsilon=-1.\)
\(\powerSum_{k}[X(1-q)] = (1-q^k)\powerSum_{k}[X]\)
\(\powerSum_{k}[X/(1-q)] = \powerSum_{k}[X]/(1-q^k)\)
\(\powerSum_{k}[X+Y] = \powerSum_{k}[X]+\powerSum_{k}[Y]\)
\(\powerSum_{\lambda}[XY] = \powerSum_{\lambda}[X]\powerSum_{\lambda}[Y]\)
\(\schurS_{\lambda}[X+Y] = \sum_{\mu \subseteq \lambda} \schurS_{\mu}[X]\schurS_{\lambda/\mu}[Y]\)
\(\schurS_\nu[XY] = \sum_{\lambda,\mu} g^{\nu}_{\lambda\mu} \schurS_\lambda(\xvec) \schurS_\mu(\yvec)\) where \(g^{\nu}_{\lambda\mu}\) are the Kronecker coefficients.
The last identity generalizes as follows: \[\schurS_\nu[f\cdot g] = \sum_{\lambda,\mu} g^{\nu}_{\lambda\mu} \schurS_\lambda[f] \schurS_\mu[g].\]
We have not found a reference for the following useful relation, but it is easy to prove. It is used in [AU20].
Proposition (Alexandersson, 2019).
Let \(f\) be a homogeneous symmetric function of degree \(n.\) Then \[\powerSum_k[ \omega f ] = (-1)^{n(k+1)}\omega(\powerSum_k[ f ]).\]
#Other identities
#Bosonic plethysm and cluster algebras
The bosonic plethysm coefficients are the multiplicities \[\schurS_\mu[\schurS_2] = \sum_\lambda a^\lambda_{\mu,(2)}\schurS_\lambda,\] equivalently the multiplicities of \(\mathbb{S}_\lambda V\) in \(\mathbb{S}_\mu(\operatorname{Sym}^2V).\)
Let \(V=\setC^\ell,\) \(W=\setC^m,\) and let \(U_V\) be a maximal unipotent subgroup of \(\GL(V).\) Y. Fan and J. Fei identify the highest-weight algebra \[R_{\ell,m} = \operatorname{Sym}(\operatorname{Sym}^2V\otimes W)^{U_V}\] with an upper cluster algebra \(\mathcal{U}(\Sigma_{\ell,m})\) having polynomial frozen coefficients [FF26]. The seed is skew-symmetrizable and admits a reddening sequence, so theta functions extending across the frozen boundary form a basis indexed by lattice points in a rational polyhedral cone \(C_{\ell,m}.\)
For a weak composition \(\alpha=(\alpha_1,\dotsc,\alpha_m),\) put \[b^\lambda_{\alpha,(2)} = \dim\operatorname{Hom}_{\GL(V)} \left( \mathbb{S}_\lambda V, \bigotimes_{r=1}^m \operatorname{Sym}^{\alpha_r}(\operatorname{Sym}^2V) \right).\] These nonnegative multiplicities are lattice-point counts in weight fibers of \(C_{\ell,m}.\) If \(\alpha^\sigma(\mu)_i=\mu_i-i+\sigma(i),\) then Jacobi–Trudi gives \[a^\lambda_{\mu,(2)} = \sum_{\sigma\in\symS_m} \operatorname{sgn}(\sigma) b^\lambda_{\alpha^\sigma(\mu),(2)}.\] Thus symmetric-square plethysm is an explicit finite alternating sum of polyhedral lattice-point counts. The construction does not yet give a positive combinatorial rule for \(a^\lambda_{\mu,(2)}\) itself.
Proposition
We have \[\completeH_k[\completeH_2] = \sum_{\mu : \text{ even }} \schurS_{\mu}\] where the sum ranges over all partitions of \(2k\) into even parts. This identity is due to D. Littlewood.
Milo Bechtloff Weising proves a wreath-product generalization of Littlewood reciprocity [Wei25]. The result gives branching multiplicities for irreducible \(G^n\rtimes \symS_n\)-representations inside highest-weight \(\mathrm{GL}_{nm}(\setC)\) representations, extending the classical Littlewood rule for the embedded symmetric group.
The SXP rule gives a formula for the plethysm [Wil18]: \[\schurS_\lambda[\powerSum_r] = \sum_{\nuvec} \sign_r(\nuvec^\ast) c^{\lambda}_{\nuvec} \schurS_{\nuvec^\ast}.\] See also the plethystic Murnaghan–Nakayama rule. W. F. Doran gives a tableau formula for \(\powerSum_\mu[\schurS_{(a)}]\) using roots of unity and a major-index-like statistic on semistandard tableaux [Dor98]. I. M. Gessel and Y. Zhuang give plethystic formulas for permutation enumeration [GZ20].
Florence Maas-Gariépy and É. Tétreault develop a tableau approach to plethysms \(\schurS_\nu[\completeH_\lambda]\) and \(\schurS_\nu[\elementaryE_\lambda]\) [MT22]. They use ribbon tableaux, lattice points in polytopes, and a Kronecker map to analyze the case where \(\nu\) is a partition of \(3\) and then extend to arbitrary \(\lambda.\)
Á. Gutiérrez and M. H. Rosas prove partial symmetries for large families of iterated plethysm coefficients [GR23]. Their flip symmetry generalizes the usual \(\omega\)-involution symmetry and is preserved by certain plethystic operations. Á. Gutiérrez, R. Orellana, F. Saliola, A. Schilling, and M. Zabrocki study bivariate generating functions for plethysm coefficients with bounded output length [GOSS+25]. They prove rationality, give an explicit \(q\)-Ehrhart-theoretic algorithm in the two-row case, and derive linear recursions for \(\mathrm{SL}_2\) plethysm coefficients. C. Bessenrodt, C. Bowman, and R. Paget classify multiplicity-free plethysms of Schur functions [BBP22]. R. Paget and M. Wildon study plethysms through representations of \(\mathrm{SL}_2(\setC)\) [PW21]. They classify several families of plethystic isomorphisms, including cases with conjugate partitions, rectangles, and partitions with at most two rows or columns. I. Pak, G. Panova, and J. P. Swanson give a positive combinatorial interpretation for plethysm coefficients \(\langle \schurS_\mu[\schurS_\nu],\schurS_\lambda\rangle\) when \(\lambda\) has at most two rows [PPS25]. Their model counts explicit marked trees and, in the case \(\mu=(n),\) also interprets corresponding rectangular Kronecker coefficients.
Proposition (See [BN21, Appendix B]).
For an indeterminate \(c,\) \[\schurS_\lambda\left[ \frac{\xvec}{1- c \xvec} \right] = \sum_{\rho} c^{|\rho|-|\lambda|} \det\left[ \binom{ \rho_j-j }{\lambda_i-i} \right] \cdot \schurS_\rho(\xvec).\] The determinant of binomial coefficients has a combinatorial interpretation, see [GV85].
Moreover, D. Yeliussizov shows that the plethysm is in fact a specialization of the canonical stable Grothendieck polynomial [Yel17]: \[\grothendieckStable^{(c,-c)}_\lambda(\xvec) = \schurS_\lambda\left[ \frac{\xvec}{1- c \xvec} \right].\]
#The s-perp trick
In [COSS+24], the authors describe in detail how to use the so-called s-perp trick in order to compute certain plethysm coefficients. This trick can also be used in many other settings. They give algorithms for monomial and Schur expansions of symmetric functions, and in several special cases these are faster than the corresponding SageMath routines.
First, define the following operator on a symmetric function \(f\): \[\schurS_\lambda^{\perp} f \coloneqq \sum_{\mu} \langle f , \schurS_\lambda \schurS_\mu \rangle \schurS_\mu.\]
Proposition
Let \(f\) and \(g\) be two homogeneous symmetric functions of degree \(d.\) Then \[\schurS_r^{\perp} f = \schurS_r^{\perp} g \text{ for all $1\leq r \leq d$}\] implies that \(f=g.\) The same holds if we replace \(\schurS_r = \completeH_r\) with \(\schurS_{1^r} = \elementaryE_r.\)
#Open problems
#Schur plethysm
Problem (See [LR10] for more info).
Let \(\lambda \vdash n\) and \(\mu \vdash m.\) Find a formula for the Schur plethysm coefficients in \[\schurS_\lambda[\schurS_\mu] = \sum_{\nu \vdash mn} p^{\nu}_{\lambda \mu} \schurS_{\nu}.\] This is a major open problem in the theory of symmetric functions and representation theory of classical groups.
Example
For example, \[\schurS_{211}[\schurS_{11}] = \schurS_{3 3 2} + \schurS_{3 2 2 1} + \schurS_{4 2 1 1} + \schurS_{2 2 2 1 1} + \schurS_{3 2 1 1 1} + \schurS_{3 1 1 1 1 1}.\]
The Schur plethysm coefficients stabilize under some operations. In [PW25] Paget and Wildon prove a general theorem, which specializes to all known stability results regarding plethysm coefficients. For example, the main stability result of [LO23] is proved.
For a partition \(\lambda,\) set \(\lambda[mn]=(mn-|\lambda|,\lambda_1,\lambda_2,\dotsc).\) S. Sarkar proves that \(\langle \completeH_n[\completeH_m],\schurS_{\lambda[mn]}\rangle\) is constant for \(m\geq\lambda_1\) and \(n\geq\lfloor(|\lambda|+\lambda_1)/2\rfloor,\) and identifies its stable value as \(\langle \schurS_\lambda,H[H-1-\completeH_1]\rangle,\) where \(H=\sum_{i\geq0}\completeH_i\) [Sar26]. For \(\lambda_1\leq4,\) the paper also gives a positive formula for this value as the number of lattice points in an explicit polytope.
#Foulkes conjecture
Foulkes conjecture [Fou50] states that \(\completeH_b[\completeH_a]-\completeH_a[\completeH_b]\) is Schur-positive whenever \(a \leq b.\) See the cycle index polynomial page for more information. É. Tétreault introduces a relation on integer partitions motivated by Schur positivity of differences of plethysms [Te20]. The restriction to one-part partitions is equivalent to the classical Foulkes conjecture, and the paper proves several properties via explicit inclusions of modules.
H. Zhu studies plethysm through orbit harmonics of loci of unordered set partitions [Zhu26]. Applying orbit harmonics to \(\Pi_{(2^a)}\) and \(\Pi_{(a^2)}\) gives graded \(\symS_{2a}\)-modules whose graded characters refine the Schur expansions of \(\completeH_a[\completeH_2]\) and \(\completeH_2[\completeH_a].\) The paper also formulates a Foulkes-type conjecture from the pair \(\Pi_{(b^a)},\) \(\Pi_{(a^b)}\) and proves the case \(b=2.\)
Example (A small orbit-harmonics refinement).
For \(a=3,\) Zhu’s graded Frobenius formulas [Zhu26, Thms. 3.3 and 3.5] give \[\operatorname{grFrob}(R(\Pi_{(2^3)});q) = \schurS_{6}+q\schurS_{42}+q^2\schurS_{222}\] and \[\operatorname{grFrob}(R(\Pi_{(3^2)});q) = \schurS_{6}+q\schurS_{42}.\] After forgetting the grading by setting \(q=1,\) these become the plethysms \[\completeH_3[\completeH_2] = \schurS_{6}+\schurS_{42}+\schurS_{222} \quad\text{and}\quad \completeH_2[\completeH_3] = \schurS_{6}+\schurS_{42}.\] Thus in this first nontrivial case of Foulkes’ conjecture, the difference is the single Schur-positive term \[\completeH_3[\completeH_2]-\completeH_2[\completeH_3] = \schurS_{222}.\]
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