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Dual Polar Graphs of Hermitian Polar Spaces

Updated 20 November 2025
  • The paper establishes the algebraic and combinatorial structure of dual polar graphs with explicit eigenvalue formulas and intersection arrays derived from Hermitian geometry.
  • It employs geometric embeddings, apartment characterizations, and Terwilliger algebra decompositions to elucidate distance-regularity and metric properties.
  • The results imply significant applications in finite geometry, coding theory, and representation theory through q-polynomial association schemes and related algebraic frameworks.

A dual polar graph of a Hermitian polar space is a distance-regular graph whose vertices correspond to maximal totally isotropic subspaces (generators) of a finite-dimensional vector space VV over GF(q2)\mathrm{GF}(q^2) equipped with a nondegenerate Hermitian form. Adjacency, combinatorial invariants, metric structure, and algebraic properties of these graphs are determined by the underlying Hermitian geometry. This structure provides a paradigmatic example of a QQ-polynomial association scheme with deep connections to buildings, representation theory, and finite geometry.

1. Construction of Hermitian Dual Polar Graphs

Given V=GF(q2)nV = \mathrm{GF}(q^2)^n with nondegenerate Hermitian form hh, the Hermitian polar space H(n1,q2)H(n-1, q^2) of rank d=n/2d = \lfloor n/2 \rfloor consists of all totally isotropic subspaces under hh. The set of dd-dimensional totally isotropic subspaces (generators) forms the vertex set Ω\Omega of the dual polar graph Γ\Gamma. Two generators X,YX,Y are adjacent if dim(XY)=d1\dim(X \cap Y) = d-1.

The resulting graph Γ\Gamma is distance-regular of diameter dd. The distance between generators XX and YY is d(X,Y)=ddim(XY)d(X, Y) = d - \dim(X \cap Y). The number of generators is Ω=i=0d1(qi+2+1)|\Omega| = \prod_{i=0}^{d-1} (q^{i+2}+1) for the case n=2dn = 2d (Witt index dd) (Ihringer et al., 2015, Qiao et al., 2017). The intersection array and eigenvalues are explicitly determined by qq and dd.

2. Apartments and Metric Characterization

Apartments in the dual polar graph correspond to subsets indexed by frames: sets of $2d$ points {p1,,p2d}\{p_1, \ldots, p_{2d}\} partitioned into dd pairs so that within each pair the points are not collinear but every other distinct pair is collinear. The family of maximal singular subspaces selecting one point from each pair is an apartment, combinatorially forming an nn-cube HdH_d as an induced subgraph (Pankov, 2010).

Pankov's metric characterization (Theorem 2) states that any isometric embedding of an mm-dimensional hypercube HmH_m into Γ\Gamma arises from an apartment (possibly within a parabolic subspace corresponding to a lower-rank polar space), and any isometric copy of HdH_d is a full apartment. The classification (Theorem 3) further asserts that every isometric embedding of a smaller dual polar graph into a larger arises from embedding into a parabolic determined by a singular subspace of requisite codimension. This rigidifies the geometry: all possible cube subgraphs with isometric distances are accounted for by geometric apartments (Pankov, 2010).

3. Combinatorial and Eigenvalue Structure

The Hermitian dual polar graph Γ\Gamma is QQ-polynomial and distance-regular, with intersection numbers: k=q[d]q2=q(q2d1)/(q21), ci=[i]q2, bi1=q[di+1]q2, ai=kbici=(q+1)([i]q2q[i1]q2),i=1,,d,\begin{aligned} k &= q \cdot [d]_{q^2} = q (q^{2d}-1)/(q^2-1), \ c_i &= [i]_{q^2}, \ b_{i-1} &= q \cdot [d-i+1]_{q^2}, \ a_i &= k - b_i - c_i = (q+1)([i]_{q^2} - q [i-1]_{q^2}), \quad i=1,\ldots,d, \end{aligned} where [m]q2=(q2m1)/(q21)[m]_{q^2} = (q^{2m}-1)/(q^2-1). The eigenvalues are

θi=q[di]q2[i]q2,i=0,1,,d\theta_i = q \cdot [d-i]_{q^2} - [i]_{q^2}, \qquad i=0,1,\ldots,d

with multiplicities given by differences of q2q^2-Gaussian coefficients (Qiao et al., 2017).

Γ\Gamma is geometric: each edge belongs to a unique Delsarte clique of size a1+2=q+2a_1+2 = q+2. The smallest eigenvalue is θd=k/(a1+1)=(q2d1+1)/(q(q+1))\theta_d = -k/(a_1+1) = -(q^{2d-1}+1)/(q(q+1)), and the graph satisfies the Krein condition with equality for a "light tail" idempotent at the minimal eigenvalue, characterizing the family among geometric $2$-bounded distance-regular graphs (Koolen et al., 2015).

4. Algebraic, Module, and Polynomial Structures

The Terwilliger (subconstituent) algebra T(x)\mathbb{T}(x) generated by adjacency and dual adjacency matrices acting on the standard module decomposes into irreducible thin modules. On each irreducible, the restrictions of adjacency and dual adjacency satisfy the Leonard pair tridiagonal relations, with split sequences and eigenparameters matching dual qq-Krawtchouk type (Worawannotai, 2012).

A fundamental correspondence is established with the quantum algebra Uq(sl2)U_q(\mathfrak{sl}_2): T(x)\mathbb{T}(x) is generated by two commuting Uq(sl2)U_q(\mathfrak{sl}_2) actions up to its center, and the spectrum and recurrences of the adjacency operator correspond to those of dual qq-Krawtchouk polynomials. In the Hermitian case, the generalized Terwilliger algebra with respect to base vertex and maximal clique admits a primary $2d$-dimensional module which realizes a rank-one nil-DAHA of type (C1,C1)(C^\vee_1, C_1), precisely encoding the dual qq-Krawtchouk polynomials and their non-symmetric versions (Lee et al., 2017).

5. Clique Classification and Metric Dimension

Erdős–Ko–Rado-type theorems describe maximal {0,1,,t}\{0,1,\ldots,t\}-cliques in the dual polar graph: for 0t<8d520 \le t < \frac{8d}{5}-2, every maximal tt-clique is the set of all generators containing a fixed totally isotropic subspace of codimension t/2t/2 (for even tt) or (t+1)/2(t+1)/2 (for odd tt). The size and structure of these cliques meet the Hoffman bound with equality, and there is a complete classification for large qq (Ihringer et al., 2015).

The metric dimension μ(Γ)\mu(\Gamma), or smallest resolving set, satisfies the upper bound

μ(Γ)qd1/2qd1/2+1q1/2+1\mu(\Gamma) \leq q^{d-1/2}\frac{q^{d-1/2}+1}{q^{1/2}+1}

where qq is the base field size and dd is the Witt index of the Hermitian form (Bailey et al., 2017). No matching lower bounds are known for arbitrary dd.

6. Characterization Theorems and Isomorphism Criteria

A detailed characterization (Qiao–Koolen) shows that under the conditions of non-bipartiteness, geometricity, diameter D4D\geq 4, c23c_2 \geq 3, and smallest eigenvalue k/2\leq -k/2, the only possible distance-regular graph with parameters matching ai=ci(q+1)a_i = c_i(q+1) for i=1,2i=1,2 and a specific relation for c3c_3 is the Hermitian dual polar graph 2A2D1(q)^2A_{2D-1}(q). These numerical identities, together with spectral information, rigidly determine the graph's isomorphism class (Qiao et al., 2017).

The light tail condition at the minimal eigenvalue provides a characterization coinciding precisely with the Hermitian dual polar graphs among distance-regular $2$-bounded graphs with the prescribed intersection array and eigenvalue structure (Koolen et al., 2015).

7. Broader Significance and Applications

Dual polar graphs of Hermitian spaces are central objects in the theory of finite geometries, combinatorics, and algebraic graph theory. Their apartments encode the cube geometry of Tits buildings, and the combinatorial embedding structure is completely dictated by the underlying geometry. Their highly regular structure underlies the classification of geometric distance-regular graphs and is instrumental in the paper of Leonard systems, qq-polynomial association schemes, and related objects in algebraic combinatorics and representation theory (Pankov, 2010, Qiao et al., 2017, Worawannotai, 2012).

These graphs serve as fertile ground for connections to quantum algebra, representation theory (via Uq(sl2)U_q(\mathfrak{sl}_2) and DAHA), and the theory of special polynomials, especially dual qq-Krawtchouk families and their non-symmetric generalizations (Lee et al., 2017, Worawannotai, 2012). Advanced applications include metric dimension calculations, clique size bounds, and explicit control over spectral properties relevant to coding theory and extremal set theory (Bailey et al., 2017, Ihringer et al., 2015).

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