#Noncommutative symmetric functions

For an introduction to noncommutative symmetric functions, we refer to [GKLL+95].

The algebra of noncommutative symmetric functions is dual to the algebra of quasisymmetric functions. These are not to be confused with symmetric functions in noncommuting variables. One convenient model is \[\mathrm{NSym}=\setZ\langle \completeH_1,\completeH_2,\dotsc\rangle,\] the free associative algebra generated by the noncommutative complete homogeneous functions. For a composition \(\alpha,\) write \(\completeH_\alpha\coloneqq \completeH_{\alpha_1}\completeH_{\alpha_2}\dotsm \completeH_{\alpha_\ell}.\) The pairing with quasisymmetric functions is normalized by \(\langle \completeH_\alpha,\qmonom_\beta\rangle=\delta_{\alpha,\beta}.\) There is a forgetful morphism \(\chi:\mathrm{NSym}\to\spaceSym\) sending \(\completeH_n\) to the ordinary complete homogeneous symmetric function.

There are therefore two complementary maps to keep in mind: \[\mathrm{NSym} \xrightarrow{\ \chi\ } \spaceSym, \qquad \mathrm{NSym} \cong \spaceQSym^\ast .\] The first map forgets noncommutativity. The second identifies NSym with the graded dual of \(\spaceQSym,\) so that every change of basis in QSym has a transpose change of basis in NSym.

E. Chen, K. Ono, and M. Mogielnicki lift the sprout symmetric function for record compositions of alternating permutations to NSym using noncommutative power sums [COM26]. Their expansion gives exact formulas for the number of alternating permutations with a prescribed record composition.

#Dual bases and the forgetful map

The basic dual pairs are: \( \text{NSym basis} \) \( \text{Dual QSym basis} \) \( \text{Image under }\chi\) \( \completeH_\alpha \) \( \qmonom_\alpha \) \( \completeH_{\alpha_1}\completeH_{\alpha_2}\dotsm \completeH_{\alpha_\ell}\) \( R_\alpha \) \( \gessel_\alpha \) \( \text{ordinary ribbon Schur function}\) \( \mathfrak S_\alpha \) \( \text{dual immaculate} \) \( \schurS_\alpha\text{ when }\alpha\text{ is a partition}\) \( \Psi_\alpha,\Phi_\alpha \) \( \qPsi_\alpha,\qPhi_\alpha \) \( \text{ordinary power-sum expressions}\) Here \(R_\alpha\) is the noncommutative ribbon basis. The ribbon basis is dual to the fundamental quasisymmetric basis, so it is the NSym side of descent-set enumerators. This is why ribbons appear naturally in the 0-Hecke categorification of QSym and NSym.

The two noncommutative power-sum bases above are dual to the two quasisymmetric power-sum bases \(\qPsi\) and \(\qPhi.\) Since \(\qPsi_\alpha\) and \(\qPhi_\alpha\) have positive expansions in the monomial quasisymmetric basis, duality gives positive expansions of \(\completeH_\alpha\) in the corresponding noncommutative power-sum bases [BDHM+20].

A. Hicks and R. McCloskey give a concrete realization of \(\mathrm{NSym}\) in noncommuting variables and derive the standard noncommutative elementary, complete, ribbon, and power-sum bases from that model [HM24]. Their account also gives combinatorial change-of-basis formulas using minimal products of transition matrices and brick tabloid statistics, paralleling the classical symmetric function picture.

J. M. Campbell introduces a lift of Stanley’s chromatic symmetric function to \(\mathrm{NSym}\) [Cam24]. For an unlabeled directed graph \(D,\) the construction gives an element \(X_D\in \mathrm{NSym}\) whose commutative image is the ordinary chromatic symmetric function of the underlying undirected graph. The lift is obtained from Stanley’s power-sum expansion using the \(\Psi\)-basis of \(\mathrm{NSym},\) and it leads to digraph-indexed generating sets for \(\mathrm{NSym}.\) Thus the orientation data is retained at the noncommutative level and then forgotten by the projection \(\chi:\mathrm{NSym}\to\spaceSym.\) L. Hao and S. Zhu show that Campbell’s chromatic noncommutative symmetric function distinguishes oriented stars, oriented double stars, and several families of oriented caterpillars and paths [HZ26]. Thus retaining the orientation before applying \(\chi\) can recover graph data lost by the ordinary chromatic symmetric function. J.-C. Novelli and J.-Y. Thibon study chromatic quasisymmetric functions inside the algebra of quasisymmetric functions in noncommuting variables [NT25]. Their work also proposes noncommutative Macdonald polynomials compatible with a Haglund–Wilson type formula and relates the construction to Yang–Baxter elements in Hecke algebras.

E. E. Allen and S. K. Mason give a combinatorial formula for the expansion of immaculate noncommutative symmetric functions in the complete homogeneous noncommutative basis [AM25]. Their model uses GBPR diagrams and tunnel hooks, extending the role played by special rim hooks in the classical inverse Kostka formula.

D. Arcis, C. Gonz{\'a}lez, and S. M{\'a}rquez study the Hopf algebra of noncommutative symmetric functions in superspace [AGM24]. They construct primitive elements, extend the elementary and power-sum families to superspace, introduce noncommutative ribbon Schur functions in superspace, and realize the Hopf algebra using trees. F. Lehner, J.-C. Novelli, and J.-Y. Thibon study combinatorial Hopf algebras in noncommutative probability [LNT20]. L. Guo, J.-Y. Thibon, and H. Yu study Hopf algebras of signed permutations, weak quasisymmetric functions, and Malvenuto–Reutenauer type structures [GTY20]. S. Zemel gives explicit antipode formulas for commutative and noncommutative \(q\)-deformations of QSym, including partial noncommutative-QSym and word-quasisymmetric variants [Zem26]. The usual QSym antipode formula is recovered by specialization.

#Noncommutative Schur functions

There are several Schur-like bases in \(\mathrm{NSym}.\) The noncommutative Schur functions of C. Bessenrodt, K. Luoto, and S. v. Willigenburg are the basis dual to the quasisymmetric Schur functions [BLW11]. Equivalently, they give a composition-indexed lift of ordinary Schur functions under the forgetful map \(\chi:\mathrm{NSym}\to\spaceSym.\) The older ribbon basis of [GKLL+95] is another fundamental Schur-like basis of \(\mathrm{NSym}.\)

#Immaculate Schur functions

The immaculate Schur functions form a composition-indexed basis of \(\mathrm{NSym}\) introduced by C. Berg, N. Bergeron, F. Saliola, L. Serrano, and M. Zabrocki [BBSS+14]. They are constructed using Bernstein-like creation operators, and the forgetful map \(\chi:\mathrm{NSym}\to\spaceSym\) sends \(\mathfrak{S}_\lambda\) to the ordinary Schur function \(\schurS_\lambda\) when \(\lambda\) is a partition.

The immaculate basis has a positive right Pieri rule and a Jacobi–Trudi type formula. Its dual basis is the dual immaculate Schur functions in QSym.

#Murnaghan–Nakayama rule

V. Tewari proves a noncommutative analogue of the classical Murnaghan–Nakayama rule for the noncommutative Schur functions of C. Bessenrodt, K. Luoto, and S. v. Willigenburg [Tew16]. The rule expands a product of a noncommutative power sum and a noncommutative Schur function into noncommutative Schur functions, with signs controlled by noncommutative border strips.

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