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Higher Lusztig Induction

Updated 8 July 2026
  • Higher Lusztig Induction is a family of geometric and homological constructions that generalize classical Deligne–Lusztig induction to finite local rings and p-adic groups.
  • It provides explicit inner product formulas and algebraisation results, including Mackey-type identities and induced models at both even and odd congruence levels.
  • Derived and categorical refinements, such as quantum group and D-module approaches, enhance its applications in representation theory and character sheaf analysis.

Higher Lusztig induction denotes a family of extensions of classical Deligne–Lusztig and Lusztig induction beyond the setting of finite reductive groups over finite fields. In the literature surveyed here, the phrase is used most directly for cohomological constructions attached to higher Deligne–Lusztig varieties over finite local rings and to parahoric quotients of pp-adic groups, where virtual representations such as RT,U,bθR_{T,U,b}^{\theta} and RL,P,rG(ψ)R_{L,P,r}^G(\psi) are defined from compactly supported \ell-adic cohomology (Chen, 2017, Yu, 16 Aug 2025). Closely related usages treat derived and categorical refinements of Lusztig induction, including derived induction equivalences for quantum groups and algebraic groups and torus-level DD-module kernels for parabolic induction and restriction (Hodge et al., 2016, Ginzburg, 2021). This suggests that “higher” refers either to passage to higher congruence level, to positive pp-adic depth, or to derived and categorical enhancement, while the unifying theme is the replacement of the classical Deligne–Lusztig correspondence by more elaborate geometric or homological machinery.

1. Terminological scope and basic framework

A common source of confusion is that the expression does not denote a single universally fixed construction across all subliteratures. The most direct uses concern higher Deligne–Lusztig theory for groups over finite quotients of discrete valuation rings and its parahoric or deep-level analogues for pp-adic groups, but several papers also use the phrase to describe derived, sheaf-theoretic, or categorical realizations of Lusztig-type induction (Yu, 16 Aug 2025, Ginzburg, 2021).

Setting Basic object Representative reference
Finite local rings RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta (Chen, 2017)
Parahoric quotients RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi (Yu, 16 Aug 2025)
Deep-level tame pp-adic theory RT,U,bθR_{T,U,b}^{\theta}0 and RT,U,bθR_{T,U,b}^{\theta}1 (Ivanov et al., 11 Jan 2026)
Derived and categorical refinements RT,U,bθR_{T,U,b}^{\theta}2, RT,U,bθR_{T,U,b}^{\theta}3, RT,U,bθR_{T,U,b}^{\theta}4 (Hodge et al., 2016, Ginzburg, 2021)

In the parahoric formulation, higher Lusztig induction is explicitly described as constructing “a broad class of virtual smooth representations of parahoric subgroups in a RT,U,bθR_{T,U,b}^{\theta}5-adic group,” and as a natural generalization of classical Lusztig induction to the RT,U,bθR_{T,U,b}^{\theta}6-adic setting (Yu, 16 Aug 2025). In the finite-local-ring formulation, the same philosophy appears through Greenberg realizations of reductive group schemes over RT,U,bθR_{T,U,b}^{\theta}7, with RT,U,bθR_{T,U,b}^{\theta}8, Lang preimages, and cohomological virtual representations (Chen, 2017).

2. Higher Deligne–Lusztig induction over finite local rings

One fundamental realization of higher Lusztig induction begins with a complete discrete valuation ring RT,U,bθR_{T,U,b}^{\theta}9, uniformizer RL,P,rG(ψ)R_{L,P,r}^G(\psi)0, quotient rings RL,P,rG(ψ)R_{L,P,r}^G(\psi)1, and a connected reductive group scheme over RL,P,rG(ψ)R_{L,P,r}^G(\psi)2. After Greenberg realization, one obtains an algebraic group RL,P,rG(ψ)R_{L,P,r}^G(\psi)3 over RL,P,rG(ψ)R_{L,P,r}^G(\psi)4 equipped with Frobenius RL,P,rG(ψ)R_{L,P,r}^G(\psi)5 such that

RL,P,rG(ψ)R_{L,P,r}^G(\psi)6

Fixing an RL,P,rG(ψ)R_{L,P,r}^G(\psi)7-stable maximal torus RL,P,rG(ψ)R_{L,P,r}^G(\psi)8, a Borel with unipotent radical RL,P,rG(ψ)R_{L,P,r}^G(\psi)9, and the Lang map \ell0, one defines for \ell1 the Deligne–Lusztig variety at page \ell2,

\ell3

and the associated virtual representation

\ell4

This family interpolates between higher Deligne–Lusztig and Gérardin-type constructions (Chen, 2017).

The endpoints of the family recover previously known objects. The paper states that when \ell5, \ell6 coincides with the higher Deligne–Lusztig representation introduced by Lusztig, and when \ell7 is even and \ell8, it coincides with Gérardin’s representation. It also notes a slight indexing inconsistency between the introduction and later notation, while emphasizing that the mathematical substance is clear: one endpoint of the family is the standard higher Deligne–Lusztig construction, and every intermediate page-\ell9 representation is compared against it (Chen, 2017).

The key theorem is an inner product formula. If DD0 is regular, then

DD1

and if DD2 is moreover in general position, then the inner product is DD3. Here regularity is the usual higher-level condition requiring DD4 to be non-trivial on every norm subgroup

DD5

for roots DD6, and general position means precisely that the Weyl-group stabilizer is trivial (Chen, 2017).

This formula gives a precise computational relation between generalized page-DD7 constructions and higher Lusztig induction. It does not identify DD8 with DD9, nor does it prove irreducibility, but it shows that under regularity the overlap is controlled exactly by a Weyl-stabilizer cardinality, and in the generic case it is minimal and nonzero. A plausible implication is that higher Lusztig induction is better viewed as a family of geometrically natural Lang-preimage constructions rather than a single isolated variety.

3. Algebraisation and induced models at even and odd level

A second major strand identifies higher Deligne–Lusztig representations with algebraically induced representations from congruence-level subgroups. At even level pp0, one defines the arithmetic radical

pp1

The paper proves that

pp2

where pp3 is the trivial extension of pp4 to pp5, and for generic pp6 one obtains

pp7

Here generic means regular, in general position, and satisfying the stabilizer condition

pp8

The paper presents this as the even-level solution to Lusztig’s algebraisation problem in the generic case (Chen et al., 2016).

The odd-level case is substantially subtler. For arbitrary level pp9, with

pp0

the all-level algebraisation theorem states that for strongly generic pp1,

pp2

At odd levels the inducing representation is no longer an inflated torus character. One first constructs a Heisenberg lift pp3 on pp4, characterized by

pp5

and then extends it to pp6 as pp7. The same paper also proves an induction formula

pp8

and gives a new proof of the regular semisimple character formula (Chen et al., 2023).

The level dependence clarifies one of the central features of higher Lusztig induction. At even level, algebraisation is controlled by a torus character on a congruence extension of pp9. At odd level, a genuinely non-abelian Heisenberg step intervenes. For RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta0, the same paper proves that regular, generic, and strongly generic are equivalent, so the stabilizer condition becomes particularly transparent in type RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta1 (Chen et al., 2023).

4. Parahoric and deep-level RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta2-adic forms

In the parahoric setting, higher Lusztig induction is defined for a RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta3-rational Levi subgroup RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta4, a parabolic RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta5, and the higher Deligne–Lusztig variety

RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta6

The associated induction functor is

RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta7

and when RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta8 it recovers classical Lusztig induction. The main theorem in the generic case is a Mackey-type scalar-product formula: RT,U,bθ=Hc(L1(FUrb,b),Q)θR_{T,U,b}^{\theta}=H_c^*(L^{-1}(FU^{r-b,b}),\overline{\mathbb Q}_\ell)_\theta9 for RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi0-generic constituents RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi1 arising from a generic toral representation of RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi2. In the elliptic-torus case this yields a decomposition

RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi3

where the RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi4 are pairwise non-isomorphic irreducible representations obtained by successive higher Lusztig inductions along a Howe factorization (Yu, 16 Aug 2025).

A complementary development gives an explicit decomposition of elliptic higher Deligne–Lusztig representations into Yu-type building blocks. If RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi5 is a Howe factorization, then previous work had shown

RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi6

The refinement identifies the geometric RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi7 with the classical Weil–Heisenberg representation RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi8 up to the Fintzen–Kaletha–Spice quadratic character and, under a mild condition on RL,P,rG(ψ)=Hc(XL,P,rG,Q)LrFψR_{L,P,r}^G(\psi)=H_c^*(X^G_{L,P,r},\overline{\mathbb Q}_\ell)\otimes_{L_r^F}\psi9, no further discrepancy: pp0 hence

pp1

Under the same mild condition on pp2, each unramified Yu type appears in the cohomology of higher Deligne–Lusztig varieties, and each unramified Kaletha regular supercuspidal representation is the compact induction of a specified higher Deligne–Lusztig representation up to a sign (Liu et al., 15 Jun 2025).

The tamely ramified deep-level theory extends this picture beyond the unramified case. For a tame elliptic torus pp3 and a character pp4 admitting a Howe factorization, one constructs a deep-level Deligne–Lusztig variety

pp5

and the virtual representation

pp6

Under a largeness condition on pp7, the comparison theorem states

pp8

and if pp9, then likewise

RT,U,bθR_{T,U,b}^{\theta}00

As a consequence, each regular irreducible supercuspidal is the compact induction of a deep-level Deligne–Lusztig representation, and more generally each irreducible supercuspidal is a direct summand of the compact induction of the cohomology of a deep-level Deligne–Lusztig variety (Ivanov et al., 11 Jan 2026).

Another RT,U,bθR_{T,U,b}^{\theta}01-adic realization appears for division algebras. For the RT,U,bθR_{T,U,b}^{\theta}02-adic Deligne–Lusztig ind-scheme RT,U,bθR_{T,U,b}^{\theta}03 attached to a division algebra RT,U,bθR_{T,U,b}^{\theta}04 of invariant RT,U,bθR_{T,U,b}^{\theta}05, and a primitive character RT,U,bθR_{T,U,b}^{\theta}06 of level RT,U,bθR_{T,U,b}^{\theta}07, the paper proves

RT,U,bθR_{T,U,b}^{\theta}08

where RT,U,bθR_{T,U,b}^{\theta}09 is the irreducible smooth representation of RT,U,bθR_{T,U,b}^{\theta}10 attached to RT,U,bθR_{T,U,b}^{\theta}11 by local Langlands and Jacquet–Langlands. This is a successful RT,U,bθR_{T,U,b}^{\theta}12-adic instance of the same general philosophy (Chan, 2015).

5. Derived and categorical reformulations

In a different direction, higher Lusztig induction appears as a derived or categorical enhancement of classical induction. One influential realization is the ABG induction theorem and its modular analogue. In the quantum case, for a Lusztig quantum enveloping algebra RT,U,bθR_{T,U,b}^{\theta}13 at a root of unity and its negative Borel part RT,U,bθR_{T,U,b}^{\theta}14, the theorem states

RT,U,bθR_{T,U,b}^{\theta}15

For a semisimple, simply connected algebraic group RT,U,bθR_{T,U,b}^{\theta}16 in characteristic RT,U,bθR_{T,U,b}^{\theta}17, the modular analogue is

RT,U,bθR_{T,U,b}^{\theta}18

Here “higher” is homological: the right derived induction functor recovers the entire bounded derived category of the principal block from a triangulated subcategory on the Borel side. The same work also notes truncation refinements for RT,U,bθR_{T,U,b}^{\theta}19 (Hodge et al., 2016).

A second realization occurs in torus-level RT,U,bθR_{T,U,b}^{\theta}20-module theory. For a connected and simply-connected complex semisimple group RT,U,bθR_{T,U,b}^{\theta}21 with maximal torus RT,U,bθR_{T,U,b}^{\theta}22, parabolic induction and restriction are made completely explicit in the case RT,U,bθR_{T,U,b}^{\theta}23. The functors are

RT,U,bθR_{T,U,b}^{\theta}24

where

RT,U,bθR_{T,U,b}^{\theta}25

The correspondence kernel is the Harish-Chandra RT,U,bθR_{T,U,b}^{\theta}26-module

RT,U,bθR_{T,U,b}^{\theta}27

and the paper proves

RT,U,bθR_{T,U,b}^{\theta}28

It also proves that the RT,U,bθR_{T,U,b}^{\theta}29-bimodule RT,U,bθR_{T,U,b}^{\theta}30 is flat as a right RT,U,bθR_{T,U,b}^{\theta}31-module, hence RT,U,bθR_{T,U,b}^{\theta}32 is RT,U,bθR_{T,U,b}^{\theta}33-exact, while

RT,U,bθR_{T,U,b}^{\theta}34

This is a highly explicit derived and kernel-theoretic model of Lusztig-type induction in the torus case (Ginzburg, 2021).

A third categorical usage appears in quiver geometry. There, Lusztig’s induction and restriction functors on equivariant derived categories realize multiplication and comultiplication in the Hall-algebra model of RT,U,bθR_{T,U,b}^{\theta}35, while derivation functors are special restriction functors. The basic induction is

RT,U,bθR_{T,U,b}^{\theta}36

and the paper proves derived refinements of the induction–restriction compatibility in the form of distinguished triangles such as

RT,U,bθR_{T,U,b}^{\theta}37

This strand does not define a new functor called higher Lusztig induction, but it treats the “higher” content as the passage from algebraic identities to functorial and triangulated statements in derived categories (Zhao, 2022).

6. Structural consequences, comparison principles, and recurring misconceptions

Several adjacent results clarify what higher Lusztig induction does and does not provide. On the Fourier-analytic side, one paper proves that for a semisimple Lie algebra RT,U,bθR_{T,U,b}^{\theta}38 over RT,U,bθR_{T,U,b}^{\theta}39, if RT,U,bθR_{T,U,b}^{\theta}40, then

RT,U,bθR_{T,U,b}^{\theta}41

and deduces Letellier’s conjectural compatibility of Fourier transform with Deligne–Lusztig induction,

RT,U,bθR_{T,U,b}^{\theta}42

This does not define a higher induction functor, but it shows that induction interacts with Fourier transform by explicit scalar laws controlled by the Weil index and the ranks of the source and target groups (Liu et al., 23 Apr 2026).

On the character-sheaf side, Lusztig induction for arbitrary RT,U,bθR_{T,U,b}^{\theta}43-stable Levi subgroups is related to parabolic induction of character sheaves and to induction on relative Weyl-group cosets. Under the weak Lusztig conjecture and a compatibility property between character sheaves and Deligne–Lusztig induction, the paper proves that if

RT,U,bθR_{T,U,b}^{\theta}44

then

RT,U,bθR_{T,U,b}^{\theta}45

It also establishes the comparison formula

RT,U,bθR_{T,U,b}^{\theta}46

which places Lusztig induction inside a relative Weyl-group induction formalism (Taylor et al., 2018).

On the Hecke-theoretic side, Lusztig induction operators for finite RT,U,bθR_{T,U,b}^{\theta}47 and RT,U,bθR_{T,U,b}^{\theta}48 are identified with Heisenberg operators on Fock space and, blockwise, with parabolic induction in cyclotomic rational double affine Hecke algebras. The core equalities are

RT,U,bθR_{T,U,b}^{\theta}49

on the finite-group side and

RT,U,bθR_{T,U,b}^{\theta}50

under the blockwise correspondence with CRDAHA category RT,U,bθR_{T,U,b}^{\theta}51. This gives a categorical and Hecke-theoretic lift of Lusztig induction on unipotent blocks (Srinivasan, 2014).

These comparison theorems also delimit the subject. A recurring misconception is that higher Lusztig induction always supplies a single universal functor together with a full Mackey formula, an explicit irreducible decomposition, and an exact equality with algebraically induced models. The literature is more stratified. The page-RT,U,bθR_{T,U,b}^{\theta}52 theory gives an inner product theorem rather than equality (Chen, 2017). The parahoric theory proves a generic scalar-product Mackey formula rather than a full operator identity (Yu, 16 Aug 2025). The all-level algebraisation theorem identifies higher Deligne–Lusztig representations with induced models for strongly generic characters, but the odd-level proof requires Heisenberg extensions and explicit sign control (Chen et al., 2023). A plausible summary is that higher Lusztig induction is best understood not as a single theorem, but as a research program whose central achievements are comparison formulas, algebraisation statements, derived realizations, and explicit decompositions in increasingly general geometric settings.

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