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Incomplete Tambara Functors

Updated 6 July 2026
  • Incomplete Tambara Functors are algebraic structures that extend Green functors by incorporating only those multiplicative norms specified by a chosen indexing system.
  • They interpolate between Green functors without extra norms and complete Tambara functors with all norms, reflecting features of N∞ ring spectra.
  • Their unique behavior is highlighted by free incomplete Tambara functors often being non-free and non-flat as Mackey functors, complicating module theory.

Incomplete Tambara functors are the algebraic structures that arise when a Green functor is endowed only with those multiplicative norms prescribed by a chosen indexing system. For a finite group GG, they interpolate between Green functors, where no nontrivial norms are present, and complete Tambara functors, where all norms are present. They were introduced as the algebraic analogue of NN_\infty ring structures, motivated in part by the fact that Bousfield localization can destroy some of the norm maps of a genuine equivariant commutative ring spectrum, so that π0\pi_0 need not carry full Tambara structure (Blumberg et al., 2016). Their later study showed that free incomplete Tambara functors behave very differently from classical free algebras: free incomplete Tambara functors are often not free, and usually not even flat, as underlying Mackey functors (Hill et al., 2021).

1. Indexing systems and polynomial categories

Let GG be a finite group. An indexing system OO is a full symmetric monoidal sub-coefficient system of finite HH-sets that contains all trivial sets, is closed under finite limits, and is closed under self-induction. Equivalently, one may work with an indexing category OO for GG, namely a wide, pullback-stable, finite coproduct complete subcategory of the category of finite GG-sets. The assignment OSetOGO \mapsto \mathrm{Set}^G_O gives an isomorphism of posets between indexing systems and wide, pullback-stable, finite coproduct-complete subcategories of the category of finite NN_\infty0-sets (Blumberg et al., 2016).

Given such an indexing category, one forms the category of polynomials with exponents in NN_\infty1, denoted NN_\infty2. Its objects are finite NN_\infty3-sets, and its morphisms are isomorphism classes of diagrams

NN_\infty4

with NN_\infty5. Every morphism admits the canonical decomposition

NN_\infty6

Here NN_\infty7, NN_\infty8, and NN_\infty9 are the restriction, transfer, and norm generators associated to a map π0\pi_00. Pullbacks and exponential diagrams govern composition, and the canonical commutation relations remain internal to π0\pi_01 because π0\pi_02 is pullback-stable (Blumberg et al., 2016).

The two extremal indexing categories are fundamental. The trivial indexing category π0\pi_03 contains only isotropy-preserving maps, and π0\pi_04-Tambara functors are Green functors. The complete indexing category π0\pi_05 yields complete Tambara functors, with all norms present (Hill et al., 2021).

2. Structure maps and reciprocity

An π0\pi_06-Tambara functor is a product-preserving functor

π0\pi_07

such that each π0\pi_08 is an abelian group, in fact a commutative ring. For an orbit π0\pi_09, GG0 is a commutative GG1-ring, where GG2 acts by conjugation. If GG3 and GG4 is the orbit map, then the structure maps are

GG5

with the norm GG6 present precisely when GG7 is admissible in GG8 (Hill et al., 2021).

The basic identities are the pullback formulas

GG9

together with the exponential-diagram identity expressing distributivity of norms over transfers. On values, these identities encode Mackey double-coset compatibility, Frobenius reciprocity for transfers,

OO0

and Tambara reciprocity for norms (Blumberg et al., 2016).

For admissible OO1, the classical formula for a norm on rings is

OO2

The incomplete setting retains exactly those norm maps and reciprocity relations that are licensed by the indexing system. This is the source of the term “incomplete”: the additive Mackey structure is still present, but multiplicative transfers occur only along admissible exponents (Blumberg et al., 2016).

3. Free objects, forgetful functors, and module theory

The Burnside category OO3 is the additive completion of the category of spans of finite OO4-sets, and a OO5-Mackey functor is an additive functor OO6. Equivalently, a Mackey functor is a product-preserving functor OO7 landing in abelian groups. Restriction along the inclusion OO8 gives the underlying Mackey functor

OO9

Thus every incomplete Tambara functor has an underlying Mackey functor, and the passage from Tambara data to Mackey data is functorial (Hill et al., 2021).

For a finite HH0-set HH1, the free HH2-Tambara functor on one generator at level HH3 is

HH4

the group completion of the represented functor. It satisfies the universal property

HH5

If HH6 is any HH7-Tambara functor, the free HH8-algebra on one generator at level HH9 is

OO0

where OO1 is the box product of Mackey functors (Hill et al., 2021).

The box product makes Mackey functors into a symmetric monoidal category with unit OO2, the Burnside Mackey functor. If OO3 is a Green functor, then an OO4-module is a Mackey functor OO5 equipped with an action map OO6. In OO7, “free” means a direct sum of OO8’s, “projective” means a summand of a free, and “flat” means exactness of OO9. Base change along a map GG0 preserves free, projective, and flat objects (Hill et al., 2021).

The category of incomplete Tambara functors is complete and cocomplete. The forgetful functor from GG1-Tambara functors to Mackey functors is strong symmetric monoidal and has a left adjoint GG2, given by left Kan extension. Change-of-indexing-system and change-of-groups functors admit adjoints as well: if GG3, there is a forgetful functor GG4 with left adjoint given by Kan extension, and for GG5, restriction GG6 has both a right adjoint GG7 and a left adjoint GG8 (Blumberg et al., 2016). For finite cyclic groups of prime order, the right adjoint to the operadic forgetful functor admits an explicit description in terms of pullbacks (Blumberg et al., 2017).

4. Freeness, flatness, and the failure of the classical analogy

Classically, free algebras are always free as modules over the base ring. In equivariant algebra, free incomplete Tambara functors play the role of free algebras and Mackey functors play the role of modules. A central result is that free incomplete Tambara functors often fail to be free as Mackey functors, and for solvable groups the precise flatness criterion is very restrictive (Hill et al., 2021).

A sufficient criterion for freeness is available. If GG9, GG0, and GG1 is admissible in GG2, then the free GG3-Tambara functor GG4 is free as an GG5-module, hence free as a Mackey functor. The proof uses the norm left adjoint GG6 and the fact that norms preserve freeness in the relevant setting (Hill et al., 2021).

The converse direction is sharper. If GG7 is flat as an GG8-module, then GG9 and OSetOGO \mapsto \mathrm{Set}^G_O0 is normal in OSetOGO \mapsto \mathrm{Set}^G_O1. Moreover, if OSetOGO \mapsto \mathrm{Set}^G_O2 is solvable, then OSetOGO \mapsto \mathrm{Set}^G_O3 is admissible in OSetOGO \mapsto \mathrm{Set}^G_O4. For solvable OSetOGO \mapsto \mathrm{Set}^G_O5, the following are equivalent:

  1. the underlying Mackey functor OSetOGO \mapsto \mathrm{Set}^G_O6 is flat;
  2. it is free;
  3. OSetOGO \mapsto \mathrm{Set}^G_O7, OSetOGO \mapsto \mathrm{Set}^G_O8 is admissible in OSetOGO \mapsto \mathrm{Set}^G_O9, and NN_\infty00 (Hill et al., 2021).

The obstruction comes from norms. The key mechanism is that norms impose nontrivial multiplicative relations tied to admissible sets, and symmetric powers appearing in Green functors lead to non-flat summands. In particular, if NN_\infty01, then NN_\infty02 is not flat. The proof reduces, after restriction and passage to cyclic NN_\infty03-groups, to the fact that for NN_\infty04, neither the constant Mackey functor nor the dual constant Mackey functor is flat (Hill et al., 2021).

This failure is asymptotically dominant. If NN_\infty05 counts pairs NN_\infty06 and NN_\infty07 counts those pairs yielding flat underlying Mackey functors, then

NN_\infty08

For solvable NN_\infty09, the bound NN_\infty10, where NN_\infty11 is the depth of the subgroup lattice, implies that free incomplete Tambara functors are almost never flat as Mackey functors (Hill et al., 2021).

5. Localization and representative examples

The global failure of flatness admits a precise localization remedy. Let NN_\infty12 denote the localization of the Burnside Tambara functor at the class NN_\infty13. Then there is an isomorphism of Tambara functors

NN_\infty14

and any NN_\infty15-module NN_\infty16 is isomorphic to the fixed point functor of its underlying module NN_\infty17. Equivalently,

NN_\infty18

In particular, for any indexing category NN_\infty19 and subgroup NN_\infty20, the localized free object NN_\infty21 is free as an NN_\infty22-module (Hill et al., 2021).

For NN_\infty23, the Burnside Tambara functor has

NN_\infty24

with NN_\infty25, transfer NN_\infty26 given by multiplication by NN_\infty27, and norm

NN_\infty28

This formula makes visible the torsion-type terms introduced by norms (Hill et al., 2021).

Small-group examples show the sharpness of the freeness criterion. For NN_\infty29, the indexing categories are NN_\infty30 and NN_\infty31; NN_\infty32 is free, while NN_\infty33 is not free. For NN_\infty34, the pattern remains sparse: freeness persists only for generators at normal subgroups with trivial restriction of NN_\infty35 and admissibility as dictated by the theorem. For the dihedral group NN_\infty36, freeness of NN_\infty37 occurs only where NN_\infty38 is normal, NN_\infty39 restricts trivially at NN_\infty40, and NN_\infty41 is admissible; after localization at NN_\infty42, all such examples become free (Hill et al., 2021).

6. Relation to NN_\infty43 ring spectra and later developments

Incomplete Tambara functors arise as NN_\infty44 of NN_\infty45 algebras. If NN_\infty46 is an NN_\infty47 operad and NN_\infty48 is an NN_\infty49-algebra in orthogonal NN_\infty50-spectra, then NN_\infty51 is an NN_\infty52-Tambara functor. The allowed norms on NN_\infty53 are exactly those prescribed by NN_\infty54. This gives the algebraic reflection of NN_\infty55 operads at the level of NN_\infty56, and it explains why Bousfield localization can produce algebraic structures lying strictly between Green functors and complete Tambara functors (Blumberg et al., 2016).

A later extension restricts additive transfers as well as multiplicative norms. In the bi-incomplete setting, one works with a compatible pair NN_\infty57 of transfer systems or indexing categories, where NN_\infty58 controls norms and NN_\infty59 controls transfers. Coefficient systems, Green functors, and full Tambara functors then become the cases NN_\infty60, NN_\infty61, and NN_\infty62, and bi-incomplete Tambara functors are characterized as NN_\infty63-commutative monoids in NN_\infty64-Mackey functors (Blumberg et al., 2021, Chan, 2022). Prime ideals and spectra have also been extended to this setting, simultaneously generalizing Lewis’s notion for Green functors and Nakaoka’s notion for Tambara functors (Balchin et al., 8 May 2026).

Homological algebra over free incomplete Tambara functors has developed in parallel. For odd primes NN_\infty65, cyclic-NN_\infty66-group-equivariant analogues of the Koszul resolution resolve the Burnside Mackey functor as a module over free incomplete Tambara functors, and for free incomplete Tambara functors whose underlying Mackey functor is projective there is an isomorphism

NN_\infty67

These constructions are used to compute Mackey functor-valued Hochschild homology for cyclic groups of odd prime order and for NN_\infty68 (Mehrle et al., 2024). By contrast, later computations over cyclic groups exhibit pathological behavior: unlike the classical polynomial ring case, where NN_\infty69 vanishes above degree one, there are examples in which Mackey functor-valued NN_\infty70 is nonvanishing in almost every degree (Mehrle et al., 2024). This suggests that incomplete Tambara functors retain the formal role of equivariant polynomial algebras while exhibiting substantially different homological behavior from their nonequivariant analogues.

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