The orbit method describes the irreducible representations of a maximal unipotent group through the coadjoint orbits of its Lie algebra, the nilradical nn of a Borel subalgebra of a simple Lie algebra gg. The extremal case — classifying the coadjoint orbits of maximal possible dimension 2μ(Φ)2\mu(\Phi) — was solved for the upper-triangular (type AA) case in Kirillov's 1962 founding paper, but a complete explicit description is still missing precisely for the orthogonal types BnB_n, DnD_n and for the exceptional type E8E_8. Over finite fields of large characteristic the problem is equivalent to explicitly describing the irreducible complex characters of maximal degree qμ(Φ)q^{\mu(\Phi)} of the maximal unipotent (Sylow pp-) subgroups of the Chevalley groups of these types. For BnB_n and DnD_n the number of such orbits is already known while the orbits themselves are not; for E8E_8 even the count is unavailable. In the published literature the problem remains open: the type-CC case is resolved by André and Neto, all simple types of rank at most 8 except E8E_8 are covered algorithmically, and for BnB_n and DnD_n only an announced but still unpublished treatment by Ignatev and Venchakov exists.

Background

The orbit method, created by A. A. Kirillov in 1962, describes the representation theory of nilpotent Lie groups through the geometry of coadjoint orbits. Let gg be a finite-dimensional simple Lie algebra over an algebraically closed field FF of characteristic zero (or of sufficiently large characteristic), let bb be a Borel subalgebra of gg (a maximal solvable subalgebra), and let n=[b,b]n=[b,b] be the nilradical of bb, i.e. its maximal nilpotent ideal. Concretely, if Φ\Phi is the root system of gg and Φ+\Phi^+ the positive roots determined by bb, then nn is spanned by the root vectors eαe_\alpha for α∈Φ+\alpha\in\Phi^+. The unipotent group N=exp⁡(n)N=\exp(n) acts on the dual space n∗n^*; this dual action is called the coadjoint action and its orbits are the coadjoint orbits. The orbit method asserts a bijection between coadjoint orbits and irreducible representations: over F=CF=\mathbb C, between coadjoint orbits and the continuous unitary irreducible representations of NN (as well as the primitive ideals of the universal enveloping algebra U(n)U(n)); over a finite field Fq\mathbb F_q of large enough characteristic, between coadjoint orbits and the complex irreducible characters of the finite group N(q)N(q). In the finite-field case an orbit of dimension 2e2e corresponds to an irreducible character of degree exactly qeq^e, so orbit classification is equivalent to the character theory of N(q)N(q), the maximal unipotent (Sylow pp-) subgroup of a Chevalley group G(q)G(q) (the group of Fq\mathbb F_q-points of a split simple algebraic group).

A complete classification of all coadjoint orbits of NN on n∗n^* is a wild problem (in the representation-theoretic sense of containing the classification of pairs of matrices up to simultaneous conjugation, hence admitting no tractable parametrization), so one studies orbits of special dimensions. The extremal case — orbits of the maximal possible dimension 2μ(Φ)2\mu(\Phi), the maximum of the dimensions of all coadjoint NN-orbits on n∗n^*, equivalently the case where qμ(Φ)q^{\mu(\Phi)} is the largest degree of an irreducible character of N(q)N(q) — goes back to Kirillov's founding paper, which classified all maximal-dimensional orbits for the strictly upper-triangular matrices (type An−1A_{n-1}). Much later, B. Kostant proved for a simple gg of any type that the coadjoint action of the full Borel group on n∗n^* has a unique Zariski-open orbit, that every NN-orbit inside this open stratum has maximal possible dimension, and constructed the cascade of orthogonal roots — a canonical set of pairwise orthogonal positive roots built recursively from the simple roots — as an explicit cross-section for these open-stratum maximal orbits. Two positive roots are orthogonal if their Killing pairing vanishes; an orthogonal subset of Φ+\Phi^+ (in the finite-group literature also called an orthogonal rook placement, by analogy with non-attacking rooks on the root diagram) is a set of pairwise orthogonal positive roots, and to each such subset together with a tuple of nonzero scalars one attaches a linear form on n∗n^*. Ignatyev proved that the orbit of such a form has a dimension computable from the Weyl group and constructed an explicit polarization for it — a subordinated subalgebra from which the orbit dimension is read off. Kostant's cascade, however, describes only the maximal orbits in the open stratum; maximal orbits lying in deeper strata require separate analysis.

The state of knowledge is type-dependent. Type An−1A_{n-1}: complete since Kirillov (1962). Type CnC_n: a classification of the maximal-dimensional orbits follows from the supercharacter theory of André and Neto — a tractable, coarser substitute for the full character theory built from sums of characters indexed by certain subsets of positive roots — and Venchakov (2026) recently gave an independent classification together with an explicit formula for the maximal-degree characters. Types BnB_n, DnD_n: the number of maximal-dimensional orbits is known from the highest-degree character counts for the orthogonal Sylow subgroups in the tradition of Marjoram, but no explicit description of the orbits themselves has been published. Exceptional types: Goodwin, Mosch and Röhrle (2016) gave an algorithm that parametrizes all coadjoint orbits and ran it for every simple group of rank at most 8 except E8E_8, and Surkov (2026) published a complete explicit classification of all orbits for F4F_4; hence E8E_8 is the one simple type for which not even a computed parametrization exists. The 2025 paper of Ignatev and Petukhov classified all orbits of dimensions 2, 4 and 6 uniformly for all classical types and, as a corollary, proved for all classical Chevalley groups the conjecture of Isaacs that the number Oe(q)O_e(q) of irreducible characters of degree qeq^e of a maximal unipotent subgroup is a polynomial in q−1q-1 with nonnegative integer coefficients, for exponents e≤3e\le 3; the same paper states explicitly that for BnB_n, DnD_n and E8E_8 a complete description of orbits of maximal dimension is still unknown. This leaves the classification of maximal-dimensional coadjoint orbits for Borel nilradicals of types BnB_n, DnD_n and E8E_8 as the surviving open core of this circle of problems.

Problem Statement

Let gg be a finite-dimensional simple Lie algebra of type BnB_n, DnD_n or E8E_8 over an algebraically closed field of characteristic zero (or of sufficiently large characteristic), let b⊂gb\subset g be a Borel subalgebra with nilradical n=[b,b]n=[b,b], and let N=exp⁡(n)N=\exp(n). Let Φ\Phi be the root system of gg, and let 2μ(Φ)2\mu(\Phi) denote the maximal possible dimension of a coadjoint NN-orbit on the dual space n∗n^*, i.e. the maximum of the orbit dimensions; equivalently, over finite fields of sufficiently large characteristic, qμ(Φ)q^{\mu(\Phi)} is the largest degree of an irreducible complex character of the finite group N(q)N(q). Give a complete explicit classification of the coadjoint orbits of NN on n∗n^* having dimension 2μ(Φ)2\mu(\Phi): an explicit list of canonical forms, uniform in the rank and labeled by subsets of the positive roots together with finitely many scalar parameters, such that every orbit of dimension 2μ(Φ)2\mu(\Phi) contains exactly one form of the list — in the same sense in which Kirillov's 1962 classification describes the type-AA case. By the orbit method over finite fields of sufficiently large characteristic, an equivalent formulation is: describe explicitly all irreducible complex characters of maximal degree qμ(Φ)q^{\mu(\Phi)} of the maximal unipotent subgroups N(q)N(q) of the Chevalley groups of types BnB_n, DnD_n and E8E_8. The classification should in particular produce, as a byproduct, the number of maximal-dimensional orbits for E8E_8, which is currently not known.

References

  1. Mikhail Ignatev, Alexey Petukhov, Coadjoint orbits of low dimension for nilradicals of Borel subalgebras in classical types, arXiv:2507.20332 (2025), DOI 10.48550/arXiv.2507.20332, https://arxiv.org/abs/2507.20332
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