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Discrete Moments of Half-Open Parallelepipeds

Updated 25 January 2026
  • Discrete moments of half-open parallelepipeds are finite sums of monomials evaluated over lattice points, serving as foundational units in Ehrhart theory and polyhedral enumeration.
  • They enable explicit computation of Ehrhart quasi-polynomials through analytic generating functions, Barnes polynomials, and torus flow methodologies.
  • Applications extend to lecture hall polytopes and bijective combinatorics, underscoring their significance in both theoretical and computational discrete geometry.

A half-open parallelepiped is a fundamental construct in contemporary combinatorial and discrete geometry, especially within the context of Ehrhart theory and polyhedral enumeration. Discrete moments of such parallelepipeds—finite sums of monomial evaluations over the lattice points they contain—have emerged as central atomic units for explicit formulas regarding Ehrhart quasi-polynomials, generating functions over polytopes, and related combinatorial invariants. This article surveys the rigorous definition, principal results, computational methodology, and applications of discrete moments of half-open parallelepipeds, including their key roles in the modern understanding of lattice-point enumeration and the polyhedral combinatorics of rational polytopes.

1. Definitions and General Framework

Let ΛRd\Lambda \subset \mathbb{R}^d denote a full-rank lattice, and let ω1,,ωdΛ\omega_1, \ldots, \omega_d \in \Lambda be linearly independent primitive edge vectors. The associated half-open parallelepiped, based at the origin, is

Π={λ1ω1++λdωd0λi<1}Rd.\Pi = \Bigl\{ \lambda_1 \omega_1 + \cdots + \lambda_d \omega_d \mid 0 \leq \lambda_i < 1 \Bigr\} \subset \mathbb{R}^d.

For any vRdv \in \mathbb{R}^d, the translate Π+v\Pi + v is considered. Discrete moments are formulated with respect to a complex direction zCdz \in \mathbb{C}^d and an auxiliary real parameter t>0t > 0, defining the kk-th discrete moment as

μk(Π,v;t,z)=pZdtv(modΠ)p,zk,\mu_k(\Pi, v; t, z) = \sum_{p \in \mathbb{Z}^d - t v\, (\bmod\, \Pi)} \langle p, z \rangle^k,

where the sum is over a finite, torus-parametrized subset of Zd\mathbb{Z}^d determined by the lattice flow through the torus Rd/Λ\mathbb{R}^d/\Lambda (Robins, 18 Jan 2026). These moments naturally extend to sums of arbitrary polynomials over the integer points in rational polytopes and underpin explicit computations in lattice-point enumeration.

2. Discrete Moments in Ehrhart Theory

Robins (Robins, 18 Jan 2026) demonstrates that the complexity of computing the Ehrhart quasi-polynomial LP(t)=tPZdL_P(t) = |tP \cap \mathbb{Z}^d| for a rational simple polytope PP can be localized to the evaluation of the corresponding discrete moments of half-open parallelepipeds at the vertices of PP. Through a combination of Brion's theorem, Barnes polynomials, and an auxiliary complex parameter zz, the formula for LP(t)L_P(t) assumes the form: LP(t)=(1)dd!vVert(P)k=0d(dk)Bk(tv,z,av)pZdtv(modΠv)p,zdk,L_P(t) = \frac{(-1)^d}{d!} \sum_{v \in \mathrm{Vert}(P)} \sum_{k=0}^d \binom{d}{k} B_k(t\langle v, z \rangle, a_v) \sum_{p \in \mathbb{Z}^d - t v\, (\bmod\, \Pi_v)} \langle p, z \rangle^{d-k}, where BkB_k denotes the kk-th Barnes polynomial and Πv\Pi_v is the half-open parallelepiped at vertex vv (Robins, 18 Jan 2026). The entire periodic and local-geometric structure of Ehrhart quasi-polynomials is thus encapsulated by these discrete moments.

Similarly, discrete moments encode sums of polynomial weights over integer points in dilates of PP: ptPZdp,zm=(1)dm!vVert(P)k=0d+m1k!(d+mk)!Bk(tv,z,av)qZdtv(modΠv)q,zd+mk.\sum_{p \in t P \cap \mathbb{Z}^d} \langle p, z \rangle^m = (-1)^d m! \sum_{v \in \mathrm{Vert}(P)} \sum_{k=0}^{d+m} \frac{1}{k!(d+m-k)!} B_k(t\langle v, z \rangle, a_v) \sum_{q \in \mathbb{Z}^d - t v\, (\bmod\, \Pi_v)} \langle q, z \rangle^{d+m-k}. Thus, discrete moments serve as the atomic units for all explicitly computable sums of polynomial expressions over lattice polytopes.

3. Torus Flows and Lattice Orbits

The connection between discrete moments and toral dynamics is manifest in the description of the summation index set. For fixed Πv\Pi_v, let ΛvZd\Lambda_v \subset \mathbb{Z}^d denote the sublattice generated by ω1(v),,ωd(v)\omega_1(v), \ldots, \omega_d(v) so that the real torus Tv=Rd/ΛvT_v = \mathbb{R}^d / \Lambda_v models the geometric structure. The "lattice flow"

LatticeFlowv(t):xxtvmodΛv\mathrm{LatticeFlow}_v(t): x \mapsto x - t v \bmod \Lambda_v

generates for each tt the intersection of the flow's trajectory with the fundamental domain Πv\Pi_v. Discrete moments μk(Πv,v;t,z)\mu_k(\Pi_v, v; t, z) sum p,zk\langle p, z \rangle^k over points in this moving lattice section; all quasi-periodic phenomena in Ehrhart theory derive from this flow structure (Robins, 18 Jan 2026).

4. Explicit Computation and Complexity Considerations

Though the reduction of Ehrhart formulas to sums over parallelepipeds is algorithmically clarifying, the corresponding half-open parallelepipeds Πv\Pi_v may contain exponentially many integer points in dd relative to the bit-lengths of generators, precluding naive polynomial-time summation. Nonetheless, it is conjectured (Robins, Conj. 6.1) that for fixed dd and kk, the discrete moments μk(Π)\mu_k(\Pi) can be computed in polynomial time in the encoding size of Π\Pi (Robins, 18 Jan 2026). Structural vanishing identities relate lower and higher moments, offering recursive avenues for efficient computation: 0=k=0m(mk)vVBk(tv,z,av)pΠvZdp,zmk0 = \sum_{k=0}^m \binom{m}{k}\sum_{v \in V} B_k(t\langle v, z \rangle, a_v) \sum_{p \in \Pi_v \cap \mathbb{Z}^d} \langle p, z \rangle^{m-k} for 0md10 \leq m \leq d-1 and integral polytopes. The use of generic zz values streamlines intermediate expressions, although final answers are independent of zz.

5. The Case of Lecture Hall Parallelepipeds and Bijective Combinatorics

For the specific case of the ss-lecture-hall simplex PsP_s and its associated half-open parallelepiped Pars\mathrm{Par}_s (Liu et al., 2012), the integer points admit a complete combinatorial parametrization via s-descents. Explicitly, disregarding the origin, vertices viv_i are defined by v1=(s1,...,sn),v2=(0,s2,...,sn),...,vn=(0,...,0,sn)v_1 = (s_1, ..., s_n), v_2 = (0, s_2, ..., s_n), ..., v_n = (0, ..., 0, s_n). The half-open parallelepiped is

Pars={c1v1++cnvn:0ci<1},\mathrm{Par}_s = \left\{ c_1 v_1 + \cdots + c_n v_n: 0 \leq c_i < 1 \right\},

and Vn=i=1n{0,...,si1}V_n = \prod_{i=1}^n \{0, ..., s_i-1\} parametrizes all its integer points. The s-descent set and the explicit bijection hs:VnParsZnh_s: V_n \to \mathrm{Par}_s \cap \mathbb{Z}^n yield closed-form expressions for all discrete moments: Mk1,...,kn(s)=xParsZnx1k1xnkn=rVni=1n(desss<i(r)si+ri)kiM_{k_1, ..., k_n}(s) = \sum_{x \in \mathrm{Par}_s \cap \mathbb{Z}^n} x_1^{k_1} \cdots x_n^{k_n} = \sum_{r \in V_n} \prod_{i=1}^n ( \operatorname{dess}_s^{<i}(r) s_i + r_i )^{k_i} where desss<i(r)\operatorname{dess}_s^{<i}(r) counts certain descent statistics of rr. This extends to explicit formulas for the lecture hall simplex's Ehrhart δ\delta-vector, with combinatorics fully encoding geometric data (Liu et al., 2012).

6. Low-Dimensional Examples

For d=1d = 1, the parallelepiped is trivial, and the classic quasi-polynomial formulas for lattice point enumeration on intervals are recovered, with moments easily computed and linked to fractional parts of rational endpoints (Robins, 18 Jan 2026). For d=2d = 2, e.g., lattice polygons, moments such as μ1(Πv;z)\mu_1(\Pi_v; z) can be written directly in terms of the geometric centroid and the parity of the midpoint, with area terms explicitly isolatable: LP(t)=Area(P)t2+(12vVv,z(1w1(v),z+1w2(v),z)(11Z2(cv)))t+1.L_P(t) = \mathrm{Area}(P)t^2 + \left( \frac{1}{2} \sum_{v \in V} \langle v, z \rangle \left( \frac{1}{\langle w_1(v), z \rangle} + \frac{1}{\langle w_2(v), z \rangle} \right) (1 - \mathbf{1}_{\mathbb{Z}^2}(c_v)) \right)t + 1. These computations exhibit the full range of combinatorial and analytic intricacy found in higher-dimensional situations.

7. Applications and Directions

Discrete moments of half-open parallelepipeds unify combinatorial enumeration, analytic generating function methods, and geometric decompositions—acting as the core arithmetic objects underlying closed-form Ehrhart and weighted lattice-point formulas (Robins, 18 Jan 2026). Through the explicit combinatorial models available in the lecture hall and similar settings (Liu et al., 2012), these moments also bridge polyhedral geometry and symmetric function theory, with ramifications for combinatorial representation theory and algebraic combinatorics. Efficient computation, algorithmic complexity, and the development of further vanishing identities remain active avenues for further research.


References:

  • “Ehrhart quasi-polynomials via Barnes polynomials and discrete moments of parallelepipeds” (Robins, 18 Jan 2026)
  • “The Lecture Hall Parallelepiped” (Liu et al., 2012)
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