#Whittaker functions

The Whittaker functions were introduced by H. Jacquet in 1967 [Jac67]. For an introduction to Whittaker functions, geometric crystals, and quantum Schubert calculus, see [Lam13]. B. Brubaker, V. Buciumas, D. Bump, and H. P. A. Gustafsson study colored vertex models for Iwahori Whittaker functions [BBBG24], as well as vertex-operator models for metaplectic Whittaker functions [BBBG20]. See also [BBL15] for the relation between Whittaker functions and Demazure operators.

Several deformations are useful in nearby combinatorics and representation theory. M. Mucciconi and L. Petrov introduce spin \(q\)-Whittaker polynomials and a deformed quantum Toda system [MP22]. G. Rahman, S. Mubeen, K. S. Nisar, and J. Choi define a \((p,q)\)-Whittaker function and record its basic identities [RMNC17].

#\(q\)-Whittaker functions

The \(q\)-Whittaker functions \(\qWhittaker_\lambda(\xvec;q)\) are eigenfunctions of the quantum Toda lattice.

For a recent survey on this topic, see [Ber24]. The \(q\)-Whittaker function \(\qWhittaker_\lambda(\xvec;q)\) can be defined in any of the following equivalent ways:

Example

For the one-box partition, the Kostka–Foulkes expansion gives \[\qWhittaker_{(1)}(\xvec;q)=\schurS_{(1)}.\]

We have \[\qWhittaker_\mu(\xvec;q) = \sum_{\lambda} K_{\lambda'\mu'}(q) \schurS_\lambda,\] where the coefficients are given by the Kostka–Foulkes polynomials. Proofs of this can be found in [Ass18, AG18], where RSK and a crystal structure are given.

See [Uhl19, AU20] and the cyclic sieving page for a cyclic sieving phenomenon on non-attacking fillings associated with \(q\)-Whittaker polynomials.

A. Borodin and S. Korotkikh introduce inhomogeneous spin \(q\)-Whittaker polynomials [BK21]. These symmetric functions generalize the \(t=0\) Macdonald polynomials and have vertex-model formulas, Cauchy-type identities, and interpolation characterizations. J. He and M. Wheeler study free-boundary \(q\)-Whittaker and Hall–Littlewood processes via six-vertex partition functions [HW25]. Their formulas include free-boundary Cauchy-type identities and probabilistic specializations of the associated vertex models. B. Brubaker, D. Bump, A. Hardt, and H. Spink introduce lattice models for double Whittaker polynomials and motivic Chern classes [BBHS25]. One boundary condition recovers motivic Chern classes and deformed Kazhdan–Lusztig \(R\)-polynomials, while another specialization recovers colored lattice models for Iwahori Whittaker functions.

#Skew \(q\)-Whittaker functions

In [AU20], a skew \(q\)-Whittaker function \(\qWhittaker_{\lambda/\mu}(\xvec;q)\) is introduced. It is symmetric and Schur-positive for partitions \(\mu \subseteq \lambda.\)

#Cauchy identities and combinatorial models

There are several recent combinatorial and probabilistic models for \(q\)-Whittaker functions. T. Imamura, M. Mucciconi, and T. Sasamoto prove a restricted Cauchy identity relating \(q\)-Whittaker and skew Schur sums in [IMS21]. In a companion paper [IMS23], they use skew RSK dynamics, Greene invariants, and affine crystals to give bijective proofs of Cauchy and Littlewood identities involving \(q\)-Whittaker polynomials. Together with T. Scrimshaw, they later introduce skew-column RSK dynamics on pairs of skew semistandard tableaux [IMSS26]. The dynamics linearizes the box-ball system, carries an affine-crystal structure, and gives Greene-type invariants and transformed Hall–Littlewood Cauchy and Littlewood identities.

P. D. Francesco and H. T. Vu derive rank recursions for \(q\)-Whittaker and Macdonald difference operators [FV26]. Powers of the \(q\)-Whittaker operator are expressed through a \(q\)-binomial distribution, while the Macdonald recursion follows from a Cauchy-determinant identity.

C. Lenart and J. Sidoli [LS21] compare three type \(A\) Whittaker formulas: an alcove-walk formula, a filling formula of Haglund–Haiman–Loehr type, and Tokuyama’s formula in terms of semistandard Young tableaux. Their comparison is organized by compression maps between the indexing objects.

S. Korotkikh [Kor22] later gives a representation theoretic interpretation and further interpolation properties for this family. Finally, T. V. Ratheesh [Rat24] constructs bijections between combinatorial models for the monomial expansions of \(q\)-Whittaker and modified Hall–Littlewood polynomials, preserving the relevant content and major-index statistics.

A. Bhattacharya explains the equality between the Haglund–Haiman–Loehr inv formula and the Ayyer–Mandelshtam–Martin quinv formula for \(q\)-Whittaker functions and modified Hall–Littlewood functions [Bha25]. The proof uses weighted Dyck path symmetric functions of E. Carlsson and A. Mellit; the two Dyck paths attached to a partition are related by the \(\zeta\) map, its inverse, and path reversal [Cor. 2.5 and Thm. 2.8, Bha25]. T. Basu and A. Bhattacharya give a standard-tableau formula for the Garsia–Remmel \(q\)-rook numbers [BB25]. They relate this formula to the coefficients appearing in \(q\)-Whittaker expansions of unicellular LLT functions.

A. Bhattacharya, T. V. Ratheesh, and S. Viswanath compare the column-strict filling model for \(q\)-Whittaker polynomials with partition-overlaid patterns indexing the Chari–Loktev basis of local Weyl modules [BRV24]. They construct weight-preserving bijections between these models which are compatible with projection, branching, and direct limits, and reinterpret the resulting data using coloured lattice paths [Thm. 2, BRV24].

#Subspace profiles over finite fields

A recent application of the \(q\)-Whittaker functions appears in [Ram26], which solves a finite-field enumeration problem posed by E. Bender, R. Coley, D. Robbins, and H. Rumsey [BCRR92]. Let \(\Delta\) be an \(n \times n\) matrix over the finite field \(\mathbb{F}_q.\) A subspace \(W \subseteq \mathbb{F}_q^n\) has \(\Delta\)-profile \(\mu=(\mu_1,\mu_2,\dotsc)\) if \[\dim(W+\Delta W+\cdots+\Delta^{j-1}W)=\mu_1+\cdots+\mu_j \qquad (j \geq 1).\] Let \(\sigma(\mu,\Delta)\) be the number of subspaces with \(\Delta\)-profile \(\mu.\)

The diagonalizable case was treated by S. Ram and M. J. Schlosser [RS26]. Their solution leads to polynomials \(b_{\mu,\nu}(q)\) with positive semistandard-tableau formulas, connections to set partition statistics, and a \(q\)-rook-theoretic interpretation. They also express the Touchard–Riordan crossing polynomial for chord diagrams in terms of \(q\)-Whittaker functions.

The key symmetric function attached to \(\Delta\) is the invariant flag generating function \(F_\Delta(\xvec).\) Suppose the \(\mathbb{F}_q[t]\)-module defined by the action of \(\Delta\) on \(\mathbb{F}_q^n\) decomposes as \[\mathbb{F}_q^n \cong \bigoplus_{i=1}^r \bigoplus_{j=1}^{\ell_i} \frac{\mathbb{F}_q[t]}{(g_i^{\lambda^i_j})},\] where the \(g_i\) are distinct monic irreducible polynomials of degrees \(d_i\) and \(\lambda^i=(\lambda^i_1,\lambda^i_2,\dotsc)\) are partitions. Then \[F_\Delta(\xvec)= \prod_{i=1}^r \hallLittlewoodH_{\lambda^i}(x_1^{d_i},x_2^{d_i},\dotsc;q^{d_i}) = \prod_{i=1}^r \powerSum_{d_i}\circ \hallLittlewoodH_{\lambda^i}(\xvec;q^{d_i}).\] Thus the primary decomposition data of \(\Delta,\) equivalently the similarity class type data of J. A. Green [Gre55], is packaged into a symmetric function built from modified Hall–Littlewood functions.

For example, a matrix with irreducible characteristic polynomial gives \(F_\Delta(\xvec)=\powerSum_n(\xvec)\); an elementary nilpotent Jordan block of size \(n\) gives \(F_\Delta(\xvec)=\completeH_n(\xvec)\); a nilpotent matrix of Jordan type \(\lambda\) gives \(F_\Delta(\xvec)=\hallLittlewoodH_\lambda(\xvec;q)\); and a matrix diagonalizable over \(\mathbb{F}_q\) with eigenspace dimensions \(\nu_1,\dotsc,\nu_r\) gives \[F_\Delta(\xvec)=\prod_{i=1}^r \qWhittaker_{(\nu_i)}(\xvec;q),\] a product of single-row \(q\)-Whittaker functions.

Let \(\widetilde{\qWhittaker}_\lambda(\xvec;q)\) denote the basis dual to the \(q\)-Whittaker basis with respect to the Hall scalar product \(\langle -,- \rangle.\) The main theorem of [Ram26] is \[\sigma(\mu,\Delta) = (-1)^{\sum_{j \geq 2}\mu_j} q^{\sum_{j \geq 2}\binom{\mu_j}{2}} \bigl\langle F_\Delta(\xvec), \widetilde{\qWhittaker}_\mu(\xvec;q)\completeH_{n-|\mu|}(\xvec) \bigr\rangle.\] When \(|\mu|=n,\) this gives a direct finite-field interpretation of the coefficients in the \(q\)-Whittaker expansion of \(F_\Delta(\xvec).\) In particular, the coefficients in the \(q\)-Whittaker expansions of \(\powerSum_n,\) \(\completeH_n,\) products of modified Hall–Littlewood functions, and products of one-row \(q\)-Whittaker functions count subspaces, up to sign and a power of \(q,\) with specified profiles for suitable operators.

For the special case \(F_\Delta(\xvec)=\powerSum_n(\xvec),\) the operator \(\Delta\) is simple, equivalently its characteristic polynomial is irreducible. S. Ram gives a symmetric-function-free proof of the corresponding subspace count, thereby rederiving the \(q\)-Whittaker expansion coefficients of \(\powerSum_n\) [Ram24]. This also gives another route to the Chen–Tseng solution of Niederreiter’s splitting-subspace problem [Cor. 2.9, Ram24].

The paper also applies this perspective to Krylov subspace methods. These methods have a long history going back to Lagrange, Euler, Gauss, Hilbert, and von Neumann, among others; see [LS13] for an overview. For an ordered set \(S=\{v_1,\dotsc,v_k\}\subseteq \mathbb{F}_q^n,\) the truncated Krylov subspace of order \(\ell\) generated by \(S\) is \[\operatorname{Kry}(\Delta,S,\ell) = \left\{ \sum_{i=1}^k f_i(\Delta)v_i : f_i\in \mathbb{F}_q[x],\ \deg f_i\lt{}\ell \right\}.\] [Thm. 7.1, Ram26] gives a Hall scalar-product formula involving dual \(q\)-Whittaker functions for the probability that a randomly chosen ordered set \(S\) of size \(k\) satisfies \(\operatorname{Kry}(\Delta,S,\ell)=\mathbb{F}_q^n.\)

#Relation with geometric RSK and crystals

The Whittaker functions show up when considering a geometric lift of RSK. There is also a notion of geometric crystals. I. Corwin, N. O'Connell, T. Seppäläinen, and N. Zygouras relate tropical combinatorics, geometric RSK, and Whittaker functions [COSZ14]. R. Chhaibi develops the Littelmann path model for geometric crystals and connects it with Whittaker functions and Brownian motion [Chh13].

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