A Kac–Grassmann reduction for supertannakian semisimplicity

Date: 6 September 2026

Mode: ATTACK

Status: superseded candidate packet; the publication audit repaired Lemma 4.1 and clarified the separability transfer. Use FPRD-supertannakian-publication-audit-2026-09-06.md and the final paper for the authoritative proof.

External review: none

Priority status: unassessed

Contents

1. Candidate theorem

Let C\mathscr C be a supertannakian category over an algebraically closed field kk of characteristic zero, and let A∈CA\in\mathscr C be a finite associative algebra object, not necessarily commutative.

Then the six conditions in Coulembier–Sherman, Theorem 3.17, are equivalent:

  1. AA is absolutely flat;
  2. Ext⁡‾A1(M,−)=0\underline{\operatorname{Ext}}^1_A(M,-)=0 for every finitely presented left AA-module MM;
  3. AA is a finite product of simple algebra objects;
  4. AA is semisimple in the internal Jacobson-radical sense;
  5. AA has no nonzero nilpotent two-sided ideal object; and
  6. the category of finitely presented AA-bimodules is rigid.

The new implication is

(5)⟹(1). (5)\Longrightarrow(1).

There is also a short direct proof of (2)⇒(5)(2)\Rightarrow(5). Together with Coulembier–Sherman’s established implications, these two arrows close their diagram.

The proof is structural rather than classificatory. After passage to the connected supergroup, a minimal invariant ideal is differentiably simple. Kac’s 1977 theorem identifies its underlying superalgebra as

S⊗^Λ(V), S\widehat\otimes\Lambda(V),

where SS is simple and Λ(V)\Lambda(V) is a Grassmann algebra. The Grassmann factor is intrinsic: it is the supercenter. It is a simple commutative algebra object, so Coulembier–Sherman’s commutative theorem makes it absolutely flat. Separability of the simple factor SS then lifts flatness to the whole algebra.

2. Reduction to an algebraic supergroup

By characteristic-zero supertannakian duality, and by the same finite-generation reduction used in Coulembier–Sherman, Section 5.5, it suffices to work in

C=Rep⁡fG \mathscr C=\operatorname{Rep}^f G

for an algebraic supergroup GG. Write H=G∘H=G^\circ. Its component group G/HG/H is finite etale in characteristic zero.

The action of GG on AA is by algebra automorphisms. Infinitesimally, h=Lie⁡H\mathfrak h=\operatorname{Lie}H acts by superderivations:

x(ab)=x(a)b+(−1)∣x∣∣a∣a x(b). x(ab)=x(a)b+(-1)^{|x||a|}a\,x(b).

For a connected algebraic supergroup in characteristic zero, a graded subspace of a rational module is HH-stable exactly when it is stable under the distribution action; on finite-dimensional modules this is generated by the Lie-superalgebra action together with the connected even group. In particular, an ideal stable under every superderivation is HH-stable.

3. Passing from GG to the connected component

Assume condition (5): AA has no nonzero nilpotent GG-stable two-sided ideal.

Lemma 3.1

There is no nonzero nilpotent HH-stable two-sided ideal in AA.

Proof. Let II be such an ideal. Every nilpotent ideal lies in the ordinary Jacobson radical J(A)J(A). Choose representatives for the finite component group G/HG/H, and form

IG=∑g∈G/HgI. I_G=\sum_{g\in G/H}gI.

The ordinary Jacobson radical is characteristic, so every summand lies in J(A)J(A). Hence IG⊆J(A)I_G\subseteq J(A) is nilpotent. It is nonzero and GG-stable, contradicting (5). □\square

This small step is important: no assertion that a sum of arbitrary nilpotent ideals is nilpotent is being used. All summands lie in the one nilpotent ideal J(A)J(A).

4. Minimal invariant ideals and Kac’s theorem

Choose a minimal nonzero HH-stable graded two-sided ideal I⊆AI\subseteq A. Its square is again HH-stable. Minimality gives

I2=0orI2=I. I^2=0\quad\text{or}\quad I^2=I.

Lemma 3.1 excludes the first case, so I2=II^2=I.

Lemma 4.1

The superalgebra II is differentiably simple in Kac’s sense.

Proof. Let 0≠J◃I0\ne J\triangleleft I be invariant under every superderivation of II. In particular, it is invariant under the restrictions of Lie⁡H\operatorname{Lie}H, so connectedness and rationality make it HH-stable. The candidate version originally invoked minimality at this point, but JJ need not be an ideal of AA. Instead form the ambient saturation AJAAJA. It is a nonzero HH-stable two-sided ideal of AA contained in II, so minimality gives AJA=IAJA=I. Since IA=AI=IIA=AI=I and I2=II^2=I,

I=I3=I(AJA)I=IJI⊆J. I=I^3=I(AJA)I=IJI\subseteq J.

Thus J=IJ=I. Since I2≠0I^2\ne0, this is exactly differentiable simplicity. □\square

Kac’s Proposition 5.1.1 now applies:

I≅S⊗^Λ(V), I\cong S\widehat\otimes\Lambda(V),

where SS is a finite-dimensional simple associative superalgebra and Λ(V)\Lambda(V) is a finite Grassmann superalgebra. The isomorphism need not be HH-equivariant; only its algebraic consequences are used.

In particular, II has an identity ee. Since II is a two-sided ideal of AA, this identity is a central idempotent of AA. Indeed, for a∈Aa\in A, both aeae and eaea lie in II, and

ae=eae=ea. ae=eae=ea.

The identity is unique, so the HH-stability of II implies that ee is HH-fixed. Therefore

A=I×(1−e)A A=I\times(1-e)A

as HH-algebras. Induction on dimension gives an algebra product

A=A1×⋯×At A=A_1\times\cdots\times A_t

in which every AiA_i is HH-simple and, as an underlying superalgebra,

Ai≅Si⊗^Λ(Vi). A_i\cong S_i\widehat\otimes\Lambda(V_i).

The finite component group permutes these factors. Taking its orbits gives a product of GG-simple algebra objects. Thus the argument already proves

(5)⟹(3). (5)\Longrightarrow(3).

This factorization uses no list of supergroups or algebra laws.

5. The Grassmann factor is intrinsic

For a superalgebra BB, write

Zs(B)={z∈B:zb=(−1)∣z∣∣b∣bz for homogeneous b∈B} Z_s(B)=\{z\in B:zb=(-1)^{|z||b|}bz\text{ for homogeneous }b\in B\}

for its supercenter.

Lemma 5.1

If SS is a finite-dimensional simple associative superalgebra over algebraically closed kk of characteristic zero, then

Zs(S)=k. Z_s(S)=k.

Proof. A nonzero homogeneous supercentral element generates a nonzero graded ideal, hence is invertible. An odd supercentral element squares to zero in characteristic different from two, so cannot be invertible. The even supercenter is therefore a finite-dimensional commutative division algebra over the algebraically closed field kk, and is kk. □\square

Expanding an element coefficientwise in Λ(Vi)\Lambda(V_i), Lemma 5.1 gives

Ci:=Zs(Ai)=1⊗^Λ(Vi). C_i:=Z_s(A_i)=1\widehat\otimes\Lambda(V_i).

So the Grassmann factor is not a choice made by Kac’s presentation. It is the canonical supercenter and is preserved by the HH-action.

Lemma 5.2

The commutative HH-algebra CiC_i is simple.

Proof. If 0≠L⊊Ci0\ne L\subsetneq C_i were an HH-stable ideal, then AiLA_iL would be a nonzero proper HH-stable two-sided ideal of AiA_i. This contradicts HH-simplicity. □\square

Coulembier–Sherman’s Theorem 6.4 and Corollary 6.6 apply to this canonical commutative algebra. They imply that every simple commutative algebra in a characteristic-zero supertannakian category is absolutely flat. Consequently,

Ci is absolutely flat in Rep⁡H. C_i\text{ is absolutely flat in }\operatorname{Rep}H.

This is the point at which the open noncommutative problem is reduced exactly to the already-settled commutative theorem.

6. Separability lifts flatness

The simple superalgebra SiS_i is separable in sVec⁡\operatorname{sVec}. One way to see this is the graded Artin–Wedderburn classification: over an algebraically closed field of characteristic zero, the simple associative superalgebras are of matrix or queer type, and both have an even bimodule section of multiplication. Equivalently, they are the central simple superalgebras over kk.

Tensoring such a section with CiC_i shows that the extension

Ci⟶Ai C_i\longrightarrow A_i

is separable after forgetting the HH-action. Equivariance of the chosen section is not required: exactness in Rep⁡H\operatorname{Rep}H is detected by the exact faithful forgetful functor to sVec⁡\operatorname{sVec}.

We record the standard transfer explicitly.

Lemma 6.1 (separable transfer)

Let C→BC\to B be a separable extension of finite superalgebras. If a right BB-module MM, restricted to CC, is flat, then MM is flat over BB.

Proof. A separability section makes

M⊗^BN M\widehat\otimes_B N

a natural direct summand of

M⊗^CN M\widehat\otimes_C N

for every left BB-module NN. Thus the first tensor functor is a natural retract of the second. A retract of an exact additive functor is exact. □\square

Let MM be any right AiA_i-module in Rep⁡H\operatorname{Rep}H. For an equivariant short exact sequence of left AiA_i-modules, restriction to CiC_i remains exact, so M⊗Ci−M\otimes_{C_i}- is exact internally. After applying the exact faithful forgetful functor, the nonequivariant separability section makes M⊗Ai−M\otimes_{A_i}- a natural retract of that exact functor. Hence it is exact, and faithful forgetting reflects the required internal exactness. No claim about arbitrary nonequivariant CiC_i-module sequences is used.

Each AiA_i is therefore absolutely flat in Rep⁡H\operatorname{Rep}H. Products are absolutely flat, and restriction

Rep⁡G⟶Rep⁡H \operatorname{Rep}G\longrightarrow\operatorname{Rep}H

is exact, faithful, and preserves relative tensor products. Hence AA is absolutely flat in Rep⁡G\operatorname{Rep}G. This proves

(5)⟹(1). \boxed{(5)\Longrightarrow(1).}

7. The Ext arrow closes directly

Lemma 7.1

For a finite algebra object in any supertannakian category,

(2)⟹(5). (2)\Longrightarrow(5).

Proof. Let R≠0R\ne0 be a nilpotent two-sided ideal object and set M=A/RM=A/R. The module MM is finite, hence finitely presented. Condition (2), applied to the extension

0⟶R⟶A⟶A/R⟶0 0\longrightarrow R\longrightarrow A\longrightarrow A/R\longrightarrow0

gives an epimorphism of internal-Hom objects

Hom⁡‾A(M,A)⟶Hom⁡‾A(M,M). \underline{\operatorname{Hom}}_A(M,A) \longrightarrow \underline{\operatorname{Hom}}_A(M,M).

Apply the exact faithful fiber functor to sVec⁡\operatorname{sVec}. Internal AA-linear Hom is the equalizer imposing the action relation, so its underlying vector space is the full space of underlying AA-linear maps. The identity of the underlying module MM therefore lifts to an underlying AA-linear section s:M→As:M\to A. No claim that this section is equivariant is needed.

Put e=s(1+R)e=s(1+R). Then

e≡1(modR),e2=e,Re=0. e\equiv1\pmod R,\qquad e^2=e,\qquad Re=0.

The idempotent 1−e1-e belongs to the nilpotent ideal RR, so 1−e=01-e=0. Thus e=1e=1, and Re=0Re=0 forces R=0R=0, a contradiction. □\square

8. Closing the implication diagram

Coulembier–Sherman, Theorem 3.17, proves

(6)⟺(1)⟹(2),(3)⟹(4)⟺(5), (6)\Longleftrightarrow(1)\Longrightarrow(2), \qquad (3)\Longrightarrow(4)\Longleftrightarrow(5),

and, because A∈CA\in\mathscr C, also (1)⇒(3)(1)\Rightarrow(3).

Sections 6 and 7 add

(5)⟹(1),(2)⟹(5). (5)\Longrightarrow(1), \qquad (2)\Longrightarrow(5).

Every condition therefore implies every other one.

9. Independent finite-dimensional control

There is a direct module-level picture behind Section 6. Since Ci=Λ(Vi)C_i=\Lambda(V_i) is a simple HH-algebra, its homogeneous-space presentation makes the infinitesimal orbit map onto the odd tangent space. For every nonzero ℓ∈Vi\ell\in V_i, choose an odd infinitesimal symmetry xx for which

u=x(ℓ)∈Λ(Vi)0ˉ u=x(\ell)\in\Lambda(V_i)_{\bar0}

has nonzero constant term, hence is a unit. On an equivariant module MM, the Leibniz identity gives

∇xLℓ+Lℓ∇x=Lu. \nabla_x L_\ell+L_\ell\nabla_x=L_u.

Therefore Lu−1∇xL_u^{-1}\nabla_x contracts multiplication by ℓ\ell. The restriction of MM to every one-generator exterior subalgebra is free. The rank-variety theorem for the exterior algebra then makes finite MM projective over Λ(Vi)\Lambda(V_i), recovering the finite part of the commutative flatness step by a different route.

This control is not needed for the formal proof, which uses Coulembier–Sherman’s stronger commutative theorem. It is retained because it checks that the reduction has the expected module-theoretic mechanism.

10. Audit obligations before publication

This ATTACK has produced a candidate resolution, not an externally checked theorem. A separate PUBLISH run must verify every bridge below against the primary literature and write out any suppressed categorical detail.

  1. Connected integration. Verify the exact statement that a finite graded ideal stable under Lie⁡H\operatorname{Lie}H is HH-stable for a connected algebraic supergroup in characteristic zero.
  2. Kac scope. Check that Proposition 5.1.1 applies to possibly nonunital finite associative superalgebras with I2≠0I^2\ne0, exactly as used for a minimal ideal.
  3. Canonical center. Audit the coefficientwise proof that Zs(S⊗^Λ(V))=Λ(V)Z_s(S\widehat\otimes\Lambda(V))=\Lambda(V), including the queer type.
  4. Separable transfer. Supply an explicit even separability section for both matrix and queer simple superalgebras, or cite a source giving the super version with identical hypotheses.
  5. Category reduction. Verify that the finite-generation reduction and restriction to G∘G^\circ preserve the exact relative tensor products used to test absolute flatness for all ind-modules.
  6. Priority and scope. Search for earlier use of Kac’s differentiably simple normal form in the absolute-flatness problem, and check the latest version of Coulembier–Sherman before any resolution claim.

A failure at any one of these points returns the work to ATTACK. No public claim of resolving Question 5.16 should be made before this audit is complete.

11. Sources and attribution

The combination of these ingredients into the proof above has not been externally reviewed. The source search found no earlier statement of this argument, but that is not a priority claim.

PUBLISH – conduct a hostile proof audit of the six obligations in Section 10. If all survive, prepare a self-contained resolution note and update the public claim ledger. If any fails, preserve the exact gap and return to ATTACK.