#Catalan symmetric functions

Catalan symmetric functions were introduced in [Che10] and [Pan10]. These functions are \(GL_\ell\)-equivariant Euler characteristics of vector bundles on the flag variety. The Catalan symmetric functions specialize to \(k\)-Schur functions, see [BMPS18].

See also J. Blasiak’s FPSAC 2023 talk [Bla23].

#Definition

Let \(R_{ij}\) be the raising operators on Schur functions, so that \[R_{ij} \schurS_{\alpha} = \schurS_{\alpha+\varepsilon_i-\varepsilon_j}.\] Here, \(\alpha\) can be a composition, and we then evaluate the Schur function using the Jacobi–Trudi formula.

A root ideal \(\Phi\) is an upper order ideal in \[\Delta_\ell^+ \coloneqq \{ (i,j) : 1 \leq i \lt j \leq \ell \}\] with the partial order relation \((a,b) \leq (c,d)\) when \(a\geq c\) and \(b \leq d.\) There are \(\catalan(\ell)\) different such order ideals, thus explaining the name.

Example

For example, \(\{ 15, 25, 35, 14, 24 \}\) is an order ideal: it is the set of entries above a Dyck path in the diagram

$ 15 $ $ 25 $ $ 35 $ $ 45 $ $ 5$ $ 14 $ $ 24 $ $ 34 $ $ 4$   $ 13 $ $ 23 $ $ 3$     $ 12 $ $ 2$       $ 1$        

See also how area sequences of length \(\ell\) are related to unit interval graphs.

Let \(\gamma \in \setZ^\ell\) and let \(\Phi\) be a root ideal. The Catalan symmetric function is then defined as \[\catalanH_{\Phi,\gamma}(\xvec;t) \coloneqq \prod_{(i,j)\in \Phi} (1-t R_{ij})^{-1}\schurS_{\gamma}(\xvec).\] Note that \[(1-tR_{ij})^{-1} = 1 + tR_{ij} + t^2 (R_{ij})^2 + t^3 (R_{ij})^3 + \dotsb\] but one only has to apply a finite number of these as \((R_{ij})^k\) kills any Schur function for sufficiently large \(k.\) By construction, \(\catalanH_{\Phi,\gamma}(\xvec;t)\) is a symmetric function.

The Catalan symmetric functions generalize the transformed Hall–Littlewood polynomials. If \(\mu\) is a partition of \(n,\) then using the full set of roots gives \[\hallLittlewoodT_{\mu}(\xvec;q) = \catalanH_{\Delta_n^+,\mu}(\xvec;q).\]

Example

For example, \(\Phi = \{ 15, 25, 35, 14, 24 \}\) and \(\gamma=(4,2,1,1,0)\) gives \[\catalanH_{\Phi,\gamma}(\xvec;t) = \schurS_{4211} + t \schurS_{431} + t \schurS_{521}\]

In [Che10], it was conjectured that \(\catalanH_{\Phi,\mu}(\xvec;t)\) is Schur-positive for any \(\Phi\) and partition \(\mu.\) This conjecture is resolved by J. Blasiak, J. Morse, and A. Pun in [BMP20]. They introduce a larger family of non-symmetric Catalan functions, the tame non-symmetric Catalan functions, \(\catalanH_{\Phi,\mu,w}(\xvec;t),\) which depend on an additional parameter \(w \in \symS_n.\) It is then proved that \(\catalanH_{\Phi,\mu,w}(\xvec;t)\) is key-positive, which then implies the Schur positivity for \(\catalanH_{\Phi,\mu}(\xvec;t).\)

#Katalan symmetric functions

In [BMS20], the authors consider a \(K\)-theoretic version of the Catalan symmetric functions, named Katalan symmetric functions, and show that this family includes the \(K\)-\(k\)-Schur functions and the usual Catalan symmetric functions.

The definition again uses raising operators, together with lowering operators. Let \(\Phi \subseteq \Delta_\ell^+\) be a root ideal, let \(M\) be a multiset on \(\{1,\dotsc,\ell\},\) and let \(\gamma \in \setZ^\ell.\) If \(g_\gamma\) denotes the determinantally extended dual stable Grothendieck function, and \(L_j g_\gamma = g_{\gamma-\varepsilon_j},\) then the Katalan symmetric function is \[\catalanH_{\Phi,M,\gamma}(\xvec) \coloneqq \prod_{j\in M}(1-L_j) \prod_{(i,j)\in \Phi}(1-R_{ij})^{-1} g_\gamma(\xvec).\] Repeated entries of \(M\) contribute repeated lowering factors.

A conjecture regarding the Katalan symmetric functions is solved in [IIN24].

#\(k\)-Schur polynomials

The \(k\)-Schur functions were introduced in [LLM03] under a different name, using the notation \(A_\mu^{(k)}[\xvec;t].\) The motivation was to provide a strong refinement of the Schur-positivity conjecture of the modified Macdonald polynomials. Several alternative definitions of \(k\)-Schur functions have since surfaced, and not all have been proved to be equivalent. For a thorough reference, see the book [LLMS+14].

For each integer \(k,\) we have the family of \(k\)-Schur functions \(\{ \kSchur^{(k)}_\lambda(\xvec) \}\) where the \(\lambda\) are \(k\)-bounded partitions, meaning that \(\lambda_1 \leq k.\) The \(k\)-Schur functions form a basis in the subring of symmetric functions, spanned by \(\completeH_1,\dotsc,\completeH_k,\) the complete homogeneous symmetric functions.

Y. Fang and X. Gao prove cases of the alternating dual Pieri rule and \(k\)-branching conjectures for closed \(k\)-Schur Katalan functions [FG25]. In particular, they prove the branching conjecture for strictly decreasing partitions. Y. Fan and X. Gao introduce weighted \(K\)-\(k\)-Schur functions inside the class of Katalan functions [FG25]. These simultaneously extend \(K\)-\(k\)-Schur functions and closed \(k\)-Schur Katalan functions, and give new cases of the \(K\)-\(k\)-Schur alternating conjecture.

In [LM07], it is shown that whenever the hook-length of \(\lambda\) is no larger than \(k,\) we have the identity \[\kSchur^{(k)}_\lambda(\xvec) = \schurS_\lambda(\xvec).\] Hence, as \(k\to \infty,\) the \(k\)-Schur functions reduce to the usual Schur functions.

#Definition

Note that there are several different, but conjecturally equivalent, definitions of \(k\)-Schur functions. We use the definition in [BMPS18], which defines the \(k\)-Schur functions as Catalan symmetric functions for special root ideals. Let \(\mu\) be a partition with at most \(\ell\) parts and \(\mu_1 \leq k.\)

Let \(\Phi_\mu \coloneqq \{ (i,j) \in \Delta_\ell^+ : k-\mu_i+i \lt j \}\) and define the \(k\)-Schur functions as \[\kSchur^{(k)}_\mu(\xvec;t) \coloneqq \catalanH_{\Phi_\mu,\mu}(\xvec;t) = \prod_{i=1}^\ell \prod_{j=k+1-\mu_i+i}^\ell (1-tR_{ij})^{-1} \schurS_\mu.\]

The specialization \(t=1\) is also called \(k\)-Schur functions, \[\kSchur^{(k)}_\mu(\xvec) \coloneqq \kSchur^{(k)}_\mu(\xvec;1).\] Most results so far concern this specialization.

Example

We have the following Schur expansions of some \(k\)-Schur functions: \[\kSchur^{(2)}_{221}(\xvec) = \schurS_{221}(\xvec)+\schurS_{311}(\xvec)+2\schurS_{320}(\xvec) +2\schurS_{410}(\xvec)+\schurS_{500}(\xvec)\] \[\kSchur^{(3)}_{221}(\xvec) = \schurS_{221}(\xvec)+\schurS_{320}(\xvec)\quad \text{ and } \quad \kSchur^{(4)}_{221}(\xvec) = \schurS_{221}(\xvec)\]

#Relation with affine Stanley symmetric functions

In [Lam06] it is shown that the \(k\)-Schur functions are dual to the affine Schur functions.

T. Ikeda, M. Shimozono, and K. Yamaguchi introduce \(K\)-theoretic double \(k\)-Schur functions as Schubert bases for the torus-equivariant \(K\)-homology of the affine Grassmannian [ISY24]. Their construction is a \(K\)-theoretic double analogue of the affine Grassmannian Schur-basis story.

M. Takigiku studies the sums \(\sum_{\mu\leq \lambda} g^{(k)}_\mu\) of \(K\)-\(k\)-Schur functions over principal order ideals in the strong Bruhat order on \(k\)-bounded partitions [Tak19]. He proves a Pieri-type formula for these sums and a \(k\)-rectangle factorization formula analogous to the usual \(k\)-Schur factorization.

#Pieri rule

L. Lapointe and J. Morse proved the following Pieri rule.

Theorem (See [Thm. 29, LM07]).

Let \(\nu\) be a \(k\)-bounded partition and \(r \leq k.\) Then \[\completeH_r \kSchur^{(k)}_\nu = \sum_{\mu \in H^k_{\nu,r}} \kSchur^{(k)}_\mu\] where \(H^k_{\nu,r}\) is a certain subset of partitions formed by adding horizontal \(r\)-strips to \(\lambda.\) More precisely, \[H^k_{\nu,r} = \{ \mu : \mu/\nu \text{ is a horizontal strip and } \mu^{(k)}/\nu^{(k)} \text{ is a vertical $r$-strip} \}.\] Here, \(\mu^{(k)}\) denotes the \(k\)-conjugate of \(\mu.\)

#Murnaghan–Nakayama rule

J. Bandlow, A. Schilling, and M. Zabrocki prove the following analog of the Murnaghan–Nakayama rule.

Theorem (See [BSZ11]).

For \(1\leq r \leq k\) and \(\lambda\) being a \(k\)-bounded partition, \[\powerSum_r \kSchur^{(k)}_\lambda = \sum_{\mu} (-1)^{\ht(\mu/\lambda)} \kSchur^{(k)}_\mu\] where the sum is over all \(k\)-bounded partitions \(\mu\) such that \(\mu/\lambda\) is a \(k\)-ribbon of size \(r.\) The definition of a \(k\)-ribbon is somewhat involved, see [BSZ11] for details.

An alternative proof is given by S. J. Lee [Thm. 10.1, Lee15], and D.-K. Nguyen [Ngu22] gives a proof in the more general setting, where a Murnaghan–Nakayama rule for \(K\text{-}k\)-Schur functions is also provided.

#Littlewood–Richardson rule

It is conjectured that the coefficients \(c^{\nu,k}_{\lambda\mu}\) in \[\kSchur^{(k)}_\lambda \kSchur^{(k)}_\mu = \sum_{\nu : \nu_1 \leq k} c^{\nu,k}_{\lambda\mu} \kSchur^{(k)}_\nu\] are all non-negative. These coefficients are 3-point Gromov–Witten invariants, see [LM08], and thus sometimes proved to be non-negative.

#Schur expansion

It was conjectured in [LM07] that the \(k\)-Schur functions are Schur-positive. A stronger statement is that the \(k\)-Schur functions expand positively into \((k+1)\)-Schur functions. This is now proved in [Thm. 2.6, BMPS19], where an explicit combinatorial expansion of \(\kSchur^{(k)}_\lambda(\xvec)\) into \(\{ \kSchur^{(k+1)}_\mu(\xvec) \}_{\mu}\) is given.

#Relation to modified Macdonald polynomials

S. Kato [Kat25] shows that Garcia–Haiman modules can be decomposed into certain modules whose characters are \(k\)-Schur functions. This implies that a modified Macdonald polynomial indexed by a \(k\)-bounded partition expands positively into \(k\)-Schur functions. That is, it can be expressed as a linear combination of \(\kSchur^{(k)}_\lambda\) with coefficients in \(\setN[q,t]\); see [Cor. 9.4, Kat25].

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