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Deep Level Deligne–Lusztig Reps

Updated 18 January 2026
  • Deep level Deligne–Lusztig representations are cohomologically-defined virtual representations that classify positive-depth supercuspidal representations of p-adic groups.
  • The construction employs geometric analogues of classical Deligne–Lusztig theory, using the cohomology of varieties over finite-level quotients tied to elliptic maximal tori.
  • The framework integrates techniques from affine Deligne–Lusztig theory and Yu–Kaletha constructions to decompose, analyze, and realize representations in varied parahoric settings.

Deep level Deligne–Lusztig representations are cohomologically-defined virtual representations of parahoric subgroups in pp-adic groups, constructed as geometric analogues and deep-level analogues of the classical Deligne–Lusztig theory for finite groups of Lie type. These constructions realize, and in many cases classify, positive-depth irreducible (supercuspidal) representations of pp-adic groups as compact inductions of geometric representations arising from the cohomology of certain infinite or finite-level varieties attached to elliptic maximal tori, often in the context of tamely ramified or unramified tori. The deep-level theory generalizes previous unramified cases and provides a geometric realization paralleling the analytic constructions of Yu and Kaletha for tame supercuspidals, with far-reaching implications for the local Langlands correspondence and the internal structure of representations of reductive pp-adic groups (Ivanov et al., 11 Jan 2026, Nie, 2024, Ivanov et al., 17 Mar 2025).

1. The Deep Level Deligne–Lusztig Construction

Let FF be a non-archimedean local field with ring of integers OF\mathcal{O}_F, maximal ideal pFp_F, and residue field kFk_F of characteristic pp; let GG be a connected reductive group over FF, splitting over a (fully general: tamely ramified) finite extension pp0. Fix an elliptic maximal torus pp1, split over pp2. For depth parameter pp3, define:

  • pp4, the "depth-pp5" smooth affine group scheme over pp6 (likewise for pp7).
  • A distinguished pro-pp8 Iwahori subgroup pp9 (the "unipotent radical" of an pp0-stable Iwahori).

Given a character pp1, define the deep level Deligne–Lusztig variety

pp2

with the pp3-adic rank-one local system pp4 on pp5 inflated from pp6. The fundamental representation is the virtual pp7-module

pp8

where pp9 and FF0 act by left and right translation, respectively (Ivanov et al., 11 Jan 2026).

2. Geometric and Cohomological Features

The cohomology FF1 is a virtual (and, under regularity/hypotheses, actual) representation of FF2, often influenced by the choice of torus FF3, the depth FF4, and the nature of FF5 (regular, generic, Howe admissible, etc.). Key facts:

  • For tamely ramified elliptic FF6 and FF7, the variety FF8 is smooth (perfect) over FF9, with dimension OF\mathcal{O}_F0 (Moy–Prasad depth).
  • The cohomology is frequently concentrated in a single degree when OF\mathcal{O}_F1 is sufficiently regular or generic (Ivanov et al., 17 Mar 2025, Ivanov et al., 2024).
  • Cohomological analysis uses Mackey formulae, Heisenberg splittings, Lagrangian subgroups (via filtration), and reductions to additive-type Deligne–Lusztig calculations.

The deep-level construction extends seamlessly to parahoric subgroups via positive loop groups and uses the Greenberg functor to parametrize finite-level quotients, enabling the realization of "higher" Deligne–Lusztig varieties as finite-type or ind-perfect schemes (Ivanov et al., 11 Jan 2026, Ivanov et al., 17 Mar 2025).

3. Decomposition and Explicit Parametrization

A crucial advance is the explicit decomposition of deep-level Deligne–Lusztig representations. For each depth-OF\mathcal{O}_F2 character OF\mathcal{O}_F3 on OF\mathcal{O}_F4 admitting a Howe factorization, there is a compact open subgroup ("Yu-type subgroup") OF\mathcal{O}_F5 and a (finite group-theoretic) Weil–Heisenberg representation OF\mathcal{O}_F6 such that:

OF\mathcal{O}_F7

where OF\mathcal{O}_F8 is the classical depth-zero Deligne–Lusztig representation attached to the Levi quotient in the factorization (Ivanov et al., 17 Mar 2025, Nie, 2024). Each irreducible constituent is thus parametrized by a refined version of Yu's data:

  • A Levi sequence OF\mathcal{O}_F9.
  • Characters and splittings attached to progressively deeper level subgroups in the filtration.
  • The geometric Weil–Heisenberg model replaces the classical, connecting pFp_F0-adic cohomology to analytic induction.

This decomposition enables a direct link between the geometry of pFp_F1 and the admissible representation-theoretic data utilized in tame supercuspidal induction.

4. Supercuspidal Realization and the Local Langlands Correspondence

Deep-level Deligne–Lusztig representations geometrically realize, or provide direct summands for, almost all irreducible supercuspidal representations of pFp_F2 in the tame (and even mildly wild) case. Explicitly:

  • For any regular elliptic pair pFp_F3 of depth pFp_F4, the compact induction

pFp_F5

recovers the corresponding Yu–Kaletha supercuspidal (Ivanov et al., 11 Jan 2026, Nie, 2024). More generally, all tame irreducible supercuspidals appear as direct summands in compact inductions from cohomology of deep-level Deligne–Lusztig varieties.

  • The trace and character formulas mirror those from the classical Deligne–Lusztig theory but now apply in the context of parahoric subgroups and deeper congruence levels.
  • Compactly induced deep-level representations match the expected local Langlands parameters via trace identities and compatibility with automorphic induction and Jacquet–Langlands transfer, as established in both the unramified and division-algebra (inner form) cases (Ivanov et al., 11 Jan 2026, Chan et al., 2018, Chan, 2015).

5. Cohomological and Orthogonality Properties

Much of the structure of deep-level Deligne–Lusztig representations is governed by:

  • Orthogonality relations: For elliptic tori pFp_F6, the induced representations satisfy strong scalar product formulas and Weyl-group-invariant orthogonality analogous to those in finite group Deligne–Lusztig theory (Chan, 2024, Dudas et al., 2020).
  • Concentration in single degree: For sufficiently generic parameters, the cohomology is concentrated and gives rise to irreducible representations, often maximal in the sense of achieving the Weil bound on rational points (Ivanov et al., 2024, Ivanov et al., 17 Mar 2025).
  • Stability phenomena: In Coxeter type and for certain torus settings, higher level unipotent representations degenerate to their level-one avatars for large pFp_F7 (Chen, 2024).

The interplay of these properties secures the irreducibility, multiplicity-free decomposition, and necessary independence from technical choices (e.g., Borel subgroup) for the representations.

6. Connections to Other Geometric and Representation-Theoretic Frameworks

Deep-level Deligne–Lusztig theory intersects with several other frameworks:

  • Kirillov's orbit method: For pro-pFp_F8 and finite pFp_F9-group quotients arising from Moy–Prasad theory, the deep-level representations coincide with those predicted by orbit method, with coadjoint orbits parametrizing irreducible modules (Ivanov et al., 2024).
  • Affine and semi-infinite Deligne–Lusztig theory: The infinite-level and semi-infinite varieties realize local Langlands and Jacquet–Langlands correspondences, embedding finite-depth constructions as components of larger ind-schemes (Takamatsu, 2023, Chan et al., 2018).
  • Parahoric and higher level constructions: The parahoric Deligne–Lusztig representations, and their orthogonality, generalize the finite-field and depth-zero cases to all positive depths, subsuming classical packets as special cases (Chan, 2024).
  • Combinatorial models: For groups like kFk_F0, flag model constructions and admissible flags afford explicit combinatorial parametrizations of nilpotent and regular orbits, further bridging algebraic and geometric perspectives (Chen, 2019).

7. Applications, Drinfeld Stratification, and Future Directions

Among the notable applications:

  • The Chan–Oi Drinfeld stratification conjecture is resolved in the context of deep-level varieties: on each kFk_F1-isotypic component, the cohomology localizes to a single "Drinfeld stratum," simplifying the decomposition (Ivanov et al., 17 Mar 2025).
  • Explicit geometric construction of Fargues–Scholze parameters for epipelagic representations is facilitated by the computation of cohomological purity and Frobenius trace formulas in this setting (Ivanov et al., 17 Mar 2025).
  • Explicit sign formulas govern the parity of the representations, with supporting evidence from Coxeter types and low rank cases (Chen, 2024).
  • The theory provides a template for extending geometric methods to more general (e.g., wild, ramified) types—though full generalization beyond tamely ramified elliptic tori remains open (Chan, 2015, Nie, 2024).

Deep-level Deligne–Lusztig representations, via the interplay of geometry, group theory, and cohomology, are now central in the structural understanding and classification of irreducible supercuspidal representations of kFk_F2-adic groups, and continue to drive connections between local harmonic analysis and arithmetic geometry (Ivanov et al., 11 Jan 2026, Ivanov et al., 17 Mar 2025, Nie, 2024).

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