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Calogero-Moser Polynomial Approximations and Dwork Congruences for Complete Flags

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Abstract

We construct pp-adic polynomial approximations to the zero-framing cohomological quasimap vertex of cotangent bundles to complete flag varieties from the trigonometric Calogero–Moser system. Negative integer couplings give regular staircase Jack polynomials with nonnegative integer coefficients. We compare them with complete-flag master polynomials extending the construction of Smirnov–Varchenko. Both families converge coefficientwise to the vertex and satisfy the full commuting equations modulo psp^s. For n≥3n\geq3, we prove sharp degree-dependent congruences and compute leading residues at every pp-power scale. Their discrepancy has coefficient norm p−1p^{-1} and an exact weighted Gauss norm giving uniform decay on smaller closed polydiscs. For the master family, multivariable Dwork congruences reconstruct the vertex by an infinite product. The results hold in every rank for 0<r/d≤1/20<r/d\leq1/2 and odd prime pp.

Introduction

Enumerative geometry of Nakajima quiver varieties relates quantum cohomology and quantum KK-theory to integrable systems [Nak94, MO19, KPSZ21, K23]. For the cotangent bundle to a complete flag variety,

Xn=T∗Fl(Cn),n≥2,X_n=T^*\mathop{\mathrm{Fl}}(\mathbb C^n),\qquad n\geq2,

the KK-theoretic vertex, with its scalar character factor, is an eigenfunction of the trigonometric Ruijsenaars–Schneider (tRS) Hamiltonians in the Kähler parameters [K21, Din21]. Its cohomological limit solves the trigonometric Calogero–Moser (tCM) equations, which also describe the quantum differential module of the Springer resolution [BMO11]. The recent work [K26] establishes compatibility of the complete-flag tRS eigenvalue problem with Frobenius action at roots of unity: partial shifts cancel in Newton–Adams combinations of the Hamiltonians, leaving the operators obtained by Frobenius action. Here we use the cohomological tCM spectral problem to construct polynomial approximations to the vertex and study their arithmetic properties.

A KK-theoretic precedent is provided by [K21] (Proposition 2.11), where a discrete specialization of framing characters truncates a normalized complete-flag vertex to a Macdonald polynomial. These polynomials occur in the correspondence between AA-type quiver varieties and ADHM moduli spaces. In the cohomological setting, polynomial solutions arise by specializing the coupling to negative integers. Choosing these integers to approach a fixed rational coupling pp-adically produces a family of exact tCM eigenfunctions at varying couplings and polynomial solutions of the fixed system modulo psp^s. After multiplication by a monomial, these terminating cohomological vertices are symmetric Jack polynomials [Mac95, NS13], the differential counterparts of the symmetric Macdonald polynomials in [K21]. We use these polynomial specializations to construct arithmetic approximations of the quasimap vertex. The spectral problem identifies the terminating vertices with Jack polynomials; our main arithmetic result compares them with the master-polynomial approximations.

A different arithmetic construction was introduced by Smirnov and Varchenko [SV23]. They express a Grassmannian vertex as a period integral of a master function, a product of rational powers of differences of auxiliary variables and Kähler parameters. Such period representations are familiar from mirror symmetry [Hori03]. The construction here uses the 3d3d mirror description of the vertex. To obtain arithmetic approximations, they replace the rational exponents by nonnegative integers approaching them pp-adically. The integrand becomes a master polynomial. Extracting a prescribed coefficient in its auxiliary variables replaces the period integral and gives a polynomial in the Kähler parameters. These polynomials satisfy Dwork congruences and reconstruct the vertex by an infinite product. We extend this construction to complete flags and prove a sharp prime-power comparison with the regular negative-parameter staircase Jack family, uniformly in rank. The two families have the same coefficientwise limit and satisfy the same full commuting equations modulo psp^s. Their difference has a degree-dependent valuation bound and explicit nonzero leading residues at every pp-power scale. These formulas describe the arithmetic of the Jack coefficients in the monomial symmetric basis and distinguish the two canonical approximation procedures.

Integrability and Polynomial Truncation

Write Q=(Q1,…,Qn−1)Q=(Q_1,\ldots,Q_{n-1}) for the Kähler parameters (Novikov variables). The vertex is a generating series of equivariant quasimap invariants of XnX_n; its coefficient in multidegree d\boldsymbol d records the corresponding curve class. Quasimaps are maps from a parametrized rational curve with finitely many base points allowed. We take the vertex with trivial insertion at the identity fixed point and normalize the source-rotation weight to one. The cotangent weight is denoted by κ\kappa. After forming the complete localization sum in each degree, we specialize the additive framing weights to zero. We prove that this specialization is regular and write

Vn(Q;κ),Vn(0;κ)=1,V_n(Q;\kappa),\qquad V_n(0;\kappa)=1,

for the resulting cohomological vertex. Each coefficient is a polynomial in κ\kappa over Q\mathbb Q. The tCM equation constructs this series recursively by formal perturbation theory around the free Hamiltonian. At any fixed Kähler degree, only finitely many perturbative terms contribute. Specializing the coupling to a negative integer then gives the terminating polynomials used below; the expansion is given in § 3.2.

Let Qi=zi/zi+1Q_i=z_i/z_{i+1}, Di=zi∂ziD_i=z_i\partial_{z_i}, and set

Hn,κ=12∑iDi2−κ(κ−1)∑i<jzizj(zi−zj)2,Jn,κ=∏i<j(1−zi/zj)κ.\begin{equation} H_{n,\kappa}=\frac12\sum_iD_i^2 -\kappa(\kappa-1)\sum_{i<j}\frac{z_iz_j}{(z_i-z_j)^2}, \qquad J_{n,\kappa}=\prod_{i<j}(1-z_i/z_j)^\kappa. \tag*{(1.1)} \end{equation}

All expressions are expanded in the chamber Q=0Q=0. The differential tRS limit gives nn commuting operators In,k(κ)\mathsf I_{n,k}(\kappa) of order kk, with principal symbols ek(ξ1,…,ξn)e_k(\xi_1,\ldots,\xi_n), where eke_k is the elementary symmetric polynomial of degree kk. The first is total momentum; on functions of the ratios QiQ_i, the second is −Hn,κ-H_{n,\kappa}. In vertex gauge we put

Bk(0)(κ)=Jn,κ−1In,k(κ)Jn,κ.\mathsf B_k^{(0)}(\kappa) =J_{n,\kappa}^{-1}\mathsf I_{n,k}(\kappa)J_{n,\kappa}.

The vertex-gauge equation Ln,κV=0\mathcal L_{n,\kappa}V=0, where Ln,κ=Jn,κ−1Hn,κJn,κ\mathcal L_{n,\kappa}=J_{n,\kappa}^{-1}H_{n,\kappa}J_{n,\kappa}, has a unique normalized formal solution in characteristic zero. We shall identify it with both the geometric vertex and the triangular chamber period. We write Pλ(α)P_\lambda^{(\alpha)} for the monic Jack polynomial with parameter α=1/κ\alpha=1/\kappa, and set Gn(z)=∏i=1nzii−1G_n(z)=\prod_{i=1}^n z_i^{i-1}.

Theorem 1.1 (Theorem 3.5 and Propositions 3.7, 3.8, 3.10, pt:joint-comparison). For every m∈Z≥0m\in\mathbb Z_{\geq0}, Fm(n)(Q):=Vn(Q;−m)∈Z[Q1,…,Qn−1],Fm(n)(0)=1.F_m^{(n)}(Q):=V_n(Q;-m)\in\mathbb Z[Q_1,\ldots,Q_{n-1}], \qquad F_m^{(n)}(0)=1. Their coefficients are nonnegative integers. For m≥1m\geq1, GnmFm(n)=Pmδ(−1/m)G_n^mF_m^{(n)}=P_{m\delta}^{(-1/m)}, where δ=(n−1,…,1,0)\delta=(n-1,\ldots,1,0). These polynomials satisfy the exact equations Bk(0)(−m)Fm(n)=0,1≤k≤n.\mathsf B_k^{(0)}(-m)F_m^{(n)}=0,\qquad 1\leq k\leq n. Fix ω=r/d\omega=r/d in lowest terms, 0<ω≤120<\omega\leq\tfrac12, and an odd prime pp. Put Ps=ps,As=ω(Ps−1),T~s(n)=FAs(n).P_s=p^s,\qquad A_s=\omega(P_s-1),\qquad \widetilde T_s^{(n)}=F_{A_s}^{(n)}. Then T~s(n)\widetilde T_s^{(n)} converges coefficientwise pp-adically to Vn(Q;ω)V_n(Q;\omega) and Bk(0)(ω)T~s(n)≡0(modps),1≤k≤n.\mathsf B_k^{(0)}(\omega)\widetilde T_s^{(n)} \equiv0\pmod{p^s},\qquad 1\leq k\leq n.

Equivalently, the vertex is the coefficientwise pp-adic limit

Vn(Q;ω)=lim⁡s→∞Gn(z)−AsPAsδ(−1/As)(z).V_n(Q;\omega) =\lim_{s\to\infty}G_n(z)^{-A_s} P_{A_s\delta}^{(-1/A_s)}(z).

Both the partition and the Jack polynomial parameter vary with ss; the normalization makes their limit a series in the fixed Kähler variables. The exact spectral equations at coupling −As-A_s and the constant coefficient one uniquely determine this polynomial family in characteristic zero. The specialization differs from the framing specialization in [K21]; the common principle is to obtain polynomial eigenfunctions from an enumerative series. For n=2n=2 this is the termination of 2F1(−m,−m;1;Q){}_2F_1(-m,-m;1;Q). In higher rank polynomiality follows from the triangular constant term and bounded external flows.

Comparison of the Two Families

The master-polynomial family is constructed from a triangular array with ii auxiliary variables in row ii, for 1≤i<n1\leq i<n, and the external variables z1,…,znz_1,\ldots,z_n in the final row. The master function multiplies a factor xω−1x^{\omega-1} for each auxiliary variable xx, a factor (x−y)2ω(x-y)^{2\omega} for each pair in the same row, and a factor (x−y)−ω(x-y)^{-\omega} for each pair in consecutive rows. A normalized integral over interlacing contours represents the vertex.

Following [SV23], we replace these exponents by nonnegative integers depending on psp^s and approaching the original exponents pp-adically. The resulting master polynomial has integral coefficients. Extracting a prescribed coefficient in its auxiliary variables and removing an external monomial gives Ts(n)T_s^{(n)}, normalized by Ts(n)(0)=1T_s^{(n)}(0)=1 and T0(n)=1T_0^{(n)}=1. Definition 2.4 specifies the exponents and coefficient extraction. The two constructions approximate the same vertex, but their polynomials need not coincide. Define their difference by

Δs(n)=T~s(n)−Ts(n).\Delta_s^{(n)}=\widetilde T_s^{(n)}-T_s^{(n)}.

For a rational number c≠0c\ne0, let vp(c)v_p(c) be the exponent of pp in cc and set ∣c∣p=p−vp(c)|c|_p=p^{-v_p(c)}, with ∣0∣p=0|0|_p=0 and vp(0)=+∞v_p(0)=+\infty. The field Qp\mathbb Q_p is the completion of Q\mathbb Q for this norm, and Zp={c∈Qp:∣c∣p≤1}\mathbb Z_p=\{c\in\mathbb Q_p:|c|_p\leq1\} is its ring of integers. On Zp[[Q]]\mathbb Z_p[[Q]] the coefficient norm is ∥∑ceQe∥p=sup⁡e∣ce∣p\|\sum c_{\boldsymbol e}Q^{\boldsymbol e}\|_p =\sup_{\boldsymbol e}|c_{\boldsymbol e}|_p. A congruence modulo psp^s means divisibility of every coefficient. Coefficientwise convergence is weaker than convergence in this norm.

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