Article identifier: Integral-Donovan-Finiteness-over-Witt-Vectors-September-25-2026

Introduction

Fix a prime pp, put k=Fpk = \mathbb{F}_p, and let O=W(k)\mathcal{O} = W(k) be its ring of Witt vectors. A block of a finite group GG over O\mathcal{O} is an algebra OGb\mathcal{O}Gb, where bb is a primitive central idempotent. Its reduction kG‾bk\overline{G}b has a defect group, well defined up to conjugacy, and we use the same defect group for the integral block. All Morita equivalences in this paper are equivalences of categories of finitely generated modules which are linear over the specified coefficient ring.

Fixing the defect group is expected to leave only finitely many Morita types of blocks. This is Donovan’s finiteness problem. Over O\mathcal{O} it concerns integral module categories, including their lattice structure, and hence is stronger than the corresponding assertion over the residue field. Our main theorem is the integral assertion for the Witt ring W(k)W(k).

Theorem 1.1. Let pp be a prime, let O=W(Fp)\mathcal{O} = W(\mathbb{F}_p), and let M≥1M \ge1 be an integer. As GG ranges over all finite groups and bb ranges over all blocks of OG\mathcal{O}G whose defect groups have order at most MM, the algebras OGb\mathcal{O}Gb belong to only finitely many O\mathcal{O}-linear Morita equivalence classes.

The theorem includes every prime, including 2, and every block, including nonprincipal blocks. The defect groups may be nonabelian; the ambient finite groups have no order bound. There are finitely many groups of order at most MM, so fixing one defect group or bounding its order gives equivalent finiteness assertions. In terms of basic orders, Theorem 1.1 says that a finite list of O\mathcal{O}-algebras represents all the indicated Morita classes.

The finiteness conclusion also passes to a fixed complete coefficient ring with algebraically closed residue field.

Corollary 1.2 (Fixed complete coefficient rings). Let pp be a prime, let RR be a fixed complete discrete valuation ring of characteristic zero whose residue field ℓ\ell is algebraically closed of characteristic pp, and let M≥1M \ge1 be an integer. As GG ranges over all finite groups and bb ranges over primitive central idempotents of RGRG for which the residue block ℓG‾b\ell\overline{G}b has a defect group of order at most MM, the algebras RGbRGb belong to only finitely many RR-linear Morita equivalence classes.

Here RR is fixed before GG and bb vary. It may be ramified, and no splitting hypothesis on its fraction field is required. The proof at the end of Section 7 uses compatible block idempotent lifts and scalar extension of the integral Morita equivalences from Theorem 1.1.

Finiteness criteria and extension methods

The local representation-theoretic questions surrounding Donovan’s conjecture were articulated in Alperin’s account of local representation theory [1]. Two different sorts of control enter finiteness: bounds on the size of a basic algebra, and bounds on its field of definition. Hiss made the field-of-definition requirement explicit: bounded defect and Cartan invariants yield Morita finiteness when the blocks have split forms over a common finite field [11], Proposition 5.1. Kessar separated these issues using Morita–Frobenius numbers [12]. For an integral order BB, its Morita–Frobenius number mfo¨⁡(B)\operatorname{mfö}(B) is the least positive coefficient-Frobenius power giving a Morita-equivalent order. The integral size and rationality bounds are combined in the finiteness theorem of Eaton–Eisele–Livesey [6], Theorem 3.10: bounded defect, bounded Cartan sum, and bounded integral Morita–Frobenius number imply integral Morita finiteness. The theorem itself allows arbitrary defect groups; the Cartan-only quasisimple reduction in that paper has the additional hypothesis of abelian defect. Their results establish integral Donovan finiteness for all abelian 2-groups [6]. For nonabelian defect groups, Eaton–Eisele–Kessar–Linckelmann–Schaeffer Fry prove integral Donovan finiteness for quaternion defect groups [5].

Crossed products encode the passage from normal subgroups to their extensions. Külshammer developed this approach in Clifford theory and in his reduction of Donovan’s conjecture [13, 14]. Eisele established integral versions and studied the relevant Picard groups [7, 8]. His geometry of rigid lattices supplies the methodological setting for integral Picard finiteness [8]. We use the preliminary Fong and nilpotent-block reduction in An–Eaton [2]; that proposition applies to arbitrary defect groups over O\mathcal{O}, independently of the extraspecial hypotheses used in their subsequent results.

For quasisimple groups, Farrell–Kessar give the uniform bound mf⁡O(B)≤4\operatorname{mf}_{\mathcal{O}}(B) \le4 [10]. Their theorem does not itself compare the multiplication factors in an arbitrary group extension. This distinction matters: controlling the Morita class of an identity component or its outer automorphisms does not determine a crossed product. Eisele–Livesey’s constructions of arbitrarily large Morita–Frobenius numbers, in families with growing defect, give further reason to retain the rationality data explicitly [9].

The companion article Donovan’s Conjecture over Algebraically Closed Fields [16] establishes bounded-defect finiteness over kk for all finite groups. It supplies two inputs here: a uniform Cartan bound, through its field theorem, and the integral extension and comparison constructions of its Sections 8 and 9. The latter retain the actual multiplication factors in the normal-subgroup extensions. Their advertised equivariance is exact after reduction. We will refine the specified integral operators to obtain exact equivariance over O\mathcal{O} itself.

What must be retained over the Witt ring

The distinction between the two coefficient rings is substantial. A coefficient-Frobenius-fixed point over O\mathcal{O} has coordinates in W(Fq)W(\mathbb{F}_q), which is infinite. Thus the finite-field point count used in a descent argument over kk gives no integral finiteness assertion. Also, a scalar obstruction over O\mathcal{O} may contain principal units, whose cohomology on a pp-group need not vanish. We address these two issues separately: the first requires rigidity of integral orders, and the second requires control of the particular scalar errors produced by the comparison.

The normal-subgroup reductions make every relevant block Morita equivalent to a block summand of a crossed order with identity component an integral block B0B_0 and grading group QQ. The integral basic orders of B0B_0 belong to a finite list, while [Q:Op′(Q)][Q:O_{p'}(Q)] is bounded. A crossed order retains both the automorphisms of B0B_0 and the units that occur when homogeneous generators are multiplied. Its restriction to a subgroup is the sum of the homogeneous components labelled by the elements of that subgroup.

Three successive assertions carry the integral proof. The first is exact comparison. The geometric overlap operators have discrepancies given by prime-to-pp character values, so these discrepancies lie in the Teichmüller subgroup T=[k×]⊆O×T=[k^\times]\subseteq\mathcal{O}^\times. We check this membership through component products, central quotients and the prescribed inner factors. Only then do we use the vanishing of positive cohomology of a finite pp-group with coefficients in TT. The resulting integral comparison extends to every Sylow restriction, giving a Morita equivalence with a bounded coefficient-Frobenius twist.

The second assertion is based finiteness. Each pure Sylow restriction is an actual finite-group block of bounded defect; we construct its group from the given automorphisms and factor elements. The field companion bounds its Cartan sum, so the integral criterion of Eaton–Eisele–Livesey gives finitely many integral Morita classes for these total restriction orders. To preserve their labelled homogeneous components and the chosen identity component, we prove an integral orbit lemma. Applied to the scheme of gradings of a fixed order with vanishing first Hochschild cohomology, it gives finitely many group-labelled gradings, even when pp divides the grading-group order. The word “fixed” refers to the total order; this is different from counting all crossed products of a fixed identity order. We retain the chosen identification of the identity component; isomorphisms preserving that identification are called based.

The third assertion removes the possibly unbounded normal p′p'-kernel of QQ while retaining those based restrictions. Its twisted group algebra splits into matrix algebras over O\mathcal{O} of degree prime to pp. Determinant-one choices of the matrices implementing a Sylow action force the new scalar discrepancy to be Teichmüller-valued. Thus the Sylow restrictions remain in their controlled based list. Restriction and corestriction control the principal-unit contribution on the remaining bounded quotient, and its Teichmüller cohomology is finite. A finite-fibre argument for the central factor systems then gives the integral Morita list.

Organization and dependencies

Section 2 fixes the crossed-product conventions and states the imported block constructions. The integral rigidity results in Section 3 are independent of the comparison construction. Section 4 proves the exact integral comparison. These two arguments meet in Section 5: the comparison gives finite total Morita types of actual extension blocks, and rigidity recovers their labelled components and markings. Section 6 removes the large normal p′p'-kernel, and Section 7 proves Theorem 1.1.

The field theorem is used before the integral theorem, in the Cartan input and the specified companion constructions. The reduction corollary records that the resulting finite integral list also represents all field basic algebras; it is not a premise of the argument. The fixed-coefficient-ring corollary is then proved by scalar extension.

Integral orders and the imported block constructions

The proof requires numerical bounds for actual blocks and a precise description of the crossed orders produced by reduction. We state these inputs separately. The distinction will matter when the numerical criterion is applied: first we identify a restriction as a group block, and then we use its Cartan and Frobenius bounds.

Orders, Frobenius and the numerical criterion

An O\mathcal{O}-order means a unital O\mathcal{O}-algebra free of finite rank as an O\mathcal{O}-module. For a general order, a block summand means its direct factor at a primitive central idempotent. Put K0=Frac⁡(O)K_0=\operatorname{Frac}(\mathcal{O}) and let σ\sigma be Witt Frobenius. For an order AA, the coefficient twist σmA\sigma^m A is the order obtained by applying σm\sigma^m to its structure constants; equivalently it is scalar transport along σm\sigma^m. For a group block we identify it with OGσm(b)\mathcal{O}G^{\sigma^m}(b). We write mf⁡O(A)\operatorname{mf}_{\mathcal{O}}(A) for the least positive mm for which AA and σmA\sigma^m A are O\mathcal{O}-linearly Morita equivalent, whenever such an mm exists. Only upper bounds for this number will be used.

Every finite O\mathcal{O}-algebra is semiperfect. A basic idempotent of a block order is a sum of one primitive idempotent for every isomorphism type of indecomposable projective. It is full, and its corner is the basic order. Basic orders are unique up to isomorphism within a Morita class. If the Cartan matrix of a block is (cij)(c_{ij}), its basic order has O\mathcal{O}-rank ∑i,jcij\sum_{i,j}c_{ij}: reduction is a split basic kk-algebra, whose dimension is that sum.

Proposition 2.1 (Cartan and integral finiteness inputs). The following assertions will be used. (i) For every pp and MM, the Cartan sums of all finite-group blocks over O\mathcal{O} with defect order at most MM are bounded by a constant c(p,M)c(p,M).

(ii) For fixed positive bounds on the defect order, Cartan sum, and integral Morita–Frobenius number, finite-group blocks over O\mathcal{O} have only finitely many O\mathcal{O}-linear Morita equivalence classes.

Proof. By [16], the reductions of the blocks in (i) have finitely many kk-Morita classes. Their Cartan matrices, up to simultaneous permutation, consequently form a finite list. Integral blocks and their reductions have the same Cartan matrix, which proves (i).

Assertion (ii) is [6], applied to the finitely many possible defect exponents. The coefficient conventions of that theorem include the absolutely unramified complete discrete valuation ring W(k)W(k) and its coefficient Frobenius, which fixes the uniformizer pp. Its defect-zero case can also be separated: a defect-zero block over W(k)W(k) is a matrix algebra over W(k)W(k) and has basic order O\mathcal{O}. Indeed, its reduction is a full matrix algebra over kk; lift its matrix units over the complete ring O\mathcal{O}, whose resulting primitive corner has rank one.

Multiplication factors and identity markings

Definition 2.2 (Crossed orders and based isomorphisms). Let RR be an O\mathcal{O}-order and QQ a finite group. A normalized crossed system consists of αq∈Aut⁡O(R)\alpha_q \in\operatorname{Aut}_{\mathcal{O}}(R) and aq,t∈R×a_{q,t} \in R^\times such that

αqαt=ad⁡(aq,t)αqt,(1)\alpha_q\alpha_t=\operatorname{ad}(a_{q,t})\alpha_{qt}, \tag*{(1)}
aq,taqt,v=αq(at,v)aq,tv,(2)a_{q,t}a_{qt,v}=\alpha_q(a_{t,v})a_{q,tv}, \tag*{(2)}

with α1=id⁡\alpha_1=\operatorname{id} and a1,q=aq,1=1a_{1,q}=a_{q,1}=1. Its crossed order is A=⨁q∈QRuqA=\bigoplus_{q\in Q}Ru_q, with

uqr=αq(r)uq,uqut=aq,tuqt,u1=1.u_qr=\alpha_q(r)u_q,\qquad u_qu_t=a_{q,t}u_{qt},\qquad u_1=1.

A QQ-labelled graded isomorphism preserves each homogeneous component with its label. When the identity component is identified with a fixed RR, such an isomorphism is based if it is the identity on RR.

Changing each uqu_q to tquqt_qu_q, with tq∈R×t_q\in R^\times and t1=1t_1=1, gives exactly the based changes of crossed systems. The induced homomorphism Q→Out⁡O(R)Q\to\operatorname{Out}_{\mathcal{O}}(R) is the outer action. It remembers the actions only modulo inner automorphisms. Both the units implementing their products in (1) and the compatibility in (2) are needed to recover the order. For S≤QS\leq Q the restriction to SS is the crossed suborder AS=⨁s∈SRusA_S=\bigoplus_{s\in S}Ru_s, with the same identity marking and the restricted factors.

Reduction and dual recovery

We call a pair (H,B)(H,B) reduced if BB is a block of OH\mathcal{O}H such that every block of a normal subgroup covered by BB is HH-stable, and

B covers a nilpotent block of H0⊴H⟹H0≤Z(H)Op(H).(3)B\text{ covers a nilpotent block of }H_0\trianglelefteq H\quad\Longrightarrow\quad H_0\leq Z(H)O_p(H). \tag*{(3)}

An–Eaton’s preliminary reduction [2] replaces an arbitrary block by a reduced pair through an O\mathcal{O}-linear basic Morita equivalence, preserving the defect group. Their coefficient conventions include O=W(k)\mathcal{O}=W(k). We apply this integral reduction directly.

The next proposition collects the group structure, actual factor elements and integral full corners supplied by the field companion. Constants in it depend only on p,Mp,M.

Proposition 2.3 (Controlled integral extensions). Let (H,B)(H,B) be a reduced pair with defect order at most MM. Put N=F∗(H)N=F^{*}(H), X=H/NX=H/N, and let bb be the block of ON\mathcal{O}N covered by BB. Then the following constructions and bounds hold.

(i) The group NN is a central product

N=PZK1⋯Kj,P=Op(H),Z=Op′(H)≤Z(H),N=P Z K_{1}\cdots K_{j},\qquad P=O_{p}(H),\qquad Z=O_{p'}(H)\leq Z(H),

where the KiK_i are quasisimple components, ∣P∣|P| and jj are bounded, and [X:Op′(X)][X:O_{p'}(X)] is bounded. The latter index is bounded also for every subgroup of every extension of XX by a p′p'-group.

(ii) There is an extension N⊴NˉN\unlhd\bar{N} with abelian p′p'-quotient A0=Nˉ/NA_{0}=\bar{N}/N. For representatives hxh_x of x∈Xx\in X, normalized by h1=1h_1=1, write hxhy=nx,yhxyh_xh_y=n_{x,y}h_{xy} with nx,y∈Nn_{x,y}\in N. Conjugation extends to automorphisms αx\alpha_x of Nˉ\bar{N} satisfying the actual identities

αxαy=ad⁡(nx,y)αxy,(4)\alpha_x\alpha_y=\operatorname{ad}(n_{x,y})\alpha_{xy}, \tag*{(4)}
nx,ynxy,z=αx(ny,z)nx,yz.(5)n_{x,y}n_{xy,z}=\alpha_x(n_{y,z})n_{x,yz}. \tag*{(5)}

Every block bˉ\bar{b} of ONˉ\mathcal{O}\bar{N} covering bb has bounded defect.

(iii) Put Ξ=Hom⁡(A0,k×)\Xi=\operatorname{Hom}(A_0,k^\times), using Teichmüller lifts of the characters over O\mathcal{O}, and Y=Ξ⋊XY=\Xi\rtimes X. There is a YY-crossed order with identity component ONˉ\mathcal{O}\bar{N} in which OH\mathcal{O}H is a full idempotent corner. After taking an appropriate central summand and a further full corner, this is a crossed order with identity component

B0=ONˉbˉB_0=\mathcal{O}\bar{N}\bar{b}

and grading group Q=Stab⁡Y(bˉ)Q=\operatorname{Stab}_{Y}(\bar{b}). In the pure XX-degrees the actions and factors are those in (ii). The index [Q:Op′(Q)][Q:O_{p'}(Q)] is bounded.

(iv) The basic orders of all these identity blocks B0B_0 belong to a finite list of integral orders R1,…,RtR_1,\ldots,R_t. Their integral Picard groups, and in particular their outer automorphism groups, are finite.

Source of the assertions. For a reduced pair, the structural conclusions follow from [16], Lemma 8.1. Its opening Morita reduction is stated over kk; we use only its conclusions about the already reduced pair, obtained here by the integral An–Eaton reduction. The compatible partial extension and its actual factors are [16], Lemma 8.2. The integral dual recovery construction and full corners are [16], Lemma 8.3.

For clarity, the dual-recovery idempotent is ∣Ξ∣−1∑χ∈Ξuχ|\Xi|^{-1}\sum_{\chi\in\Xi}u_\chi. The characters are trivial on every nx,y∈Nn_{x,y}\in N, so the pure XX-units preserve this idempotent and retain exactly these factors. This explains why the construction is integral and why it retains the multiplication data needed later. Finally (iv) is the integral assertion of [16], Lemma 8.5, using the trivial-subgroup case of its Proposition 9.1. The finite Picard assertion is also [8], Theorem B and Corollary 1.2.

Every pp-subgroup SS of YY can be conjugated by an element of Ξ\Xi into the pure subgroup XX. Indeed, its image in XX is a pp-group, and Schur–Zassenhaus conjugates the two complements to Ξ\Xi in the inverse image of that group. In the crossed order this conjugation is implemented by an integral homogeneous unit; it also transports bˉ\bar{b}. We may therefore work with pure pp-subgroups, provided we keep the transported identity block in the same family. In particular, the orders of the relevant pp-subgroups of QQ are bounded: their intersection with Op′(Q)O_{p'}(Q) is trivial, so they inject into the quotient whose order was bounded in (iii).

There is no bound here on the orders of the central kernels in the universal-cover presentations, or on the extra central pp-factors used in the partial regular extensions. The comparison in Section 4 descends through those kernels before any bounded-defect integral criterion is applied.

The companion’s comparison data

The comparison convention in [16] uses an integral Morita bimodule but asserts exact covariance and factor identities on its reduction. We use the particular integral operators constructed there. Their ingredients have four distinct roles. Lemmas 9.2–9.4 realize the genuine field, graph and inner relations, construct an invariant torus and character, and choose a common parabolic–Levi pair with the specified inner overlap. Lemma 9.5 gives an integral Levi Morita bimodule with strict geometric actions and matching central actions. Lemma 9.6 gives a uniformly bounded coefficient-Frobenius return and its prime-to-pp character twist. Finally, Lemma 9.7 computes the integral scalar overlap of the chosen operators.

Section 4 recalls these constructions with their exact hypotheses and shows that their scalar errors stay in T\mathcal{T}. The subsequent normalization over O\mathcal{O} is proved here. Thus the imported comparison supplies operators and overlap identities, while Proposition 4.2 supplies the exact integral factor law required by the later extension argument.

Integral orbits and gradings of a fixed order

An ungraded Morita list does not specify the components of a crossed order. This section gives the additional rigidity needed to recover both their group labels and the identity marking. There are three steps: an orbit lemma over O\mathcal{O}, a tangent calculation for gradings of a fixed total order, and a rank argument which passes from Morita classes to such fixed orders. The orbit method is related to the geometry of rigid lattices and Picard groups in [8]; the grading argument below works for every finite grading group.

Integral orbit finiteness

Lemma 3.1 (Integral orbit finiteness). Let JJ be a smooth affine group scheme of finite type over O\mathcal{O}, acting on an affine scheme VV of finite type over O\mathcal{O}. For x∈V(O)x \in V(\mathcal{O}) let TxVT_xV denote the integral tangent module along the section xx. The points for which the orbit derivative

Lie⁡(J)⟶TxV\operatorname{Lie}(J) \longrightarrow T_xV

is surjective belong to only finitely many J(O)J(\mathcal{O})-orbits.

Proof. We bound the special-fibre orbits and then cut each one by a fixed integral slice. The latter has only finitely many possible generic points arising from the sections under consideration.

The integral tangent and horizontal components. Embed VV as a closed subscheme of AOr\mathbb{A}_{\mathcal{O}}^r, with finitely many defining equations. The module TxVT_xV is the kernel of their Jacobian map on Or\mathcal{O}^r. It is therefore saturated in Or\mathcal{O}^r. Write u=rank⁡K0TxVu = \operatorname{rank}_{K_0} T_xV. Surjectivity of the orbit derivative and saturation imply that its coordinate matrix has a unit minor of size uu. This follows, for example, from Smith normal form over the discrete valuation ring O\mathcal{O}.

After extension to K0K_0, this derivative has rank uu, which is also dim⁡K0TxK0VK0\dim_{K_0} T_{x_{K_0}}V_{K_0}. Every irreducible component of VK0V_{K_0} through xK0x_{K_0} consequently has dimension at most uu. Let VuV_u be the reduced closure in VV of the union of the generic-fibre irreducible components of dimension at most uu. There are finitely many such components. Each of their horizontal closures has special fibre of dimension at most its generic-fibre dimension. This is the dimension theorem for an irreducible finite-type scheme over a valuation ring [20].

Thus

dim⁡(Vu)k≤u.(6)\dim(V_u)_k \leq u. \tag*{(6)}

The section xx factors through VuV_u, because its generic point does and O↪K0\mathcal{O} \hookrightarrow K_0 is injective.

The special-fibre orbits. Let x0x_0 be the reduction of xx. The unit minor remains nonzero modulo pp, so the special-fibre orbit of x0x_0 has dimension at least uu. This orbit lies in (Vu)k(V_u)_k. One way to verify that last assertion is to lift every element of J(k)J(k) to J(O)J(\mathcal{O}), using smoothness and completeness, and then apply it to the section xx. The transformed generic point still lies on components of dimension at most uu. Equation (6) now shows that the orbit has dimension exactly uu.

A locally closed orbit of dimension uu in a scheme of dimension at most uu contains an open subset of an irreducible component of dimension uu. Two distinct orbits cannot both contain dense open subsets of the same component. There are therefore finitely many possible special-fibre orbits for this uu.

A fixed Hensel slice. Fix one such orbit and a representative x0x_0. By lifting elements of J(k)J(k), move all integral points under consideration so that their reduction equals x0x_0. Choose uu coordinate functions whose orbit derivative has a nonzero uu-minor at x0x_0, and fix integral lifts a1,…,aua_1,\ldots,a_u of their values there. For each such integral point xx, the map

J⟶AOu,g⟼the selected coordinates of gxJ \longrightarrow\mathbb{A}^u_{\mathcal{O}}, \qquad g \longmapsto\text{the selected coordinates of }gx

is smooth near the identity: JJ is smooth and its relative differential there is surjective. Hensel lifting supplies g≡1(modp)g \equiv1 \pmod p for which the selected coordinates of gxgx are exactly the aia_i. Thus every integral orbit has a representative in the fixed affine slice

W=V∩{selected coordinates=a1,…,au}.W = V \cap\{\text{selected coordinates}=a_1,\ldots,a_u\}.

For any resulting point yy, the selected-coordinate differential is an isomorphism on TyK0VK0T_{y_{K_0}}V_{K_0}: that space has dimension uu, and the same minor is a unit since yy reduces to x0x_0. It follows that TyK0WK0=0T_{y_{K_0}}W_{K_0}=0. Such a point is isolated in the finite-type K0K_0-scheme WK0W_{K_0}. A noetherian scheme has only finitely many isolated points. Each generic point gives at most one integral section, again by the injection O↪K0\mathcal{O} \hookrightarrow K_0. Hence there are finitely many representatives in this slice. Taking the finite union over the special-fibre orbits and the possible ranks 0≤u≤r0 \leq u \leq r proves the lemma.

The integral tangent module in this proof need not reduce to the whole tangent space at x0x_0. Saturation and the unit minor are what the proof uses. In particular, no smoothness assumption on VV, nor on an automorphism scheme occurring as VV, is needed. The rank-zero case is included by using no slice coordinates. The argument uses smoothness of JJ for lifting and for its differential; it does not require JJ to be connected.

Block rigidity and labelled gradings

Lemma 3.2 (Hochschild rigidity and outer automorphisms). Let AA be an O\mathcal{O}-order Morita equivalent to a finite direct sum of finite-group block orders. Then HHO1(A)=0\mathrm{HH}^{1}_{\mathcal{O}}(A)=0, and Out⁡O(A)\operatorname{Out}_{\mathcal{O}}(A) is finite.

Proof. For a finite group GG, the conjugation permutation lattice and Shapiro’s lemma give

HHO1(OG)≅H1(G,OGconj)≅⨁[g]H1(CG(g),O)=0.\mathrm{HH}^{1}_{\mathcal{O}}(\mathcal{O}G) \cong H^{1}(G,\mathcal{O}G_{\mathrm{conj}}) \cong\bigoplus_{[g]} H^{1}(C_G(g),\mathcal{O})=0.

The action on the last coefficient module is trivial, and Hom⁡(CG(g),Oadd)=0\operatorname{Hom}(C_G(g),\mathcal{O}_{\mathrm{add}})=0 because CG(g)C_G(g) is finite and O\mathcal{O} is torsion-free. Hochschild cohomology splits over finite direct products and is Morita invariant, proving the first assertion. Thus every O\mathcal{O}-linear derivation of AA is inner.

The unit group scheme A×A^\times is an open subscheme of the affine space underlying AA, defined by invertibility of the regular-representation determinant. It is smooth. The automorphisms of AA form an affine scheme of finite type: impose the multiplicative and unital equations on an invertible linear map. Let A×A^\times act by postcomposition with inner automorphisms. At an automorphism, compose with its inverse to identify the tangent module with the derivations of AA. The orbit derivative then consists of the inner derivations, so it is surjective. Lemma 3.1 says exactly that there are finitely many cosets modulo inner automorphisms. □

Theorem 3.3 (Gradings of a fixed integral order). Let AA be an O\mathcal{O}-order with HH⁡O1(A)=0\operatorname{HH}^{1}_{\mathcal{O}}(A)=0, and let HH be any fixed finite group. There are only finitely many HH-labelled gradings of AA up to O\mathcal{O}-algebra automorphism. In fact there are only finitely many orbits under inner automorphisms.

Proof. We apply Lemma 3.1 to the space of decompositions compatible with multiplication. The key point is that the tangent calculation uses cancellation in HH, without averaging over HH.

A grading A=⨁h∈HAhA=\bigoplus_{h\in H}A_h is specified by its orthogonal projections eh∈End⁡O(A)e_h\in\operatorname{End}_{\mathcal{O}}(A). These satisfy

ehej=δh,jeh,∑h∈Heh=1,e_h e_j=\delta_{h,j}e_h,\qquad\sum_{h\in H}e_h=1,
eh(1A)=δh,11A,el(eg(x)eh(y))=0(l≠gh).e_h(1_A)=\delta_{h,1}1_A,\qquad e_l(e_g(x)e_h(y))=0\quad(l\ne gh).

The last equations need only be imposed on a fixed finite basis of AA. They define an affine finite-type grading scheme, on which A×A^\times acts by conjugation.

We compute its integral tangent module at a grading. A first-order deformation of the direct-sum decomposition is uniquely represented by an off-diagonal O\mathcal{O}-linear map δ:A→A\delta:A\to A, where

ehδeh=0(h∈H).e_h\delta e_h=0\quad(h\in H).

The deformed summands are (1+εδ)Ah(1+\varepsilon\delta)A_h over O[ε]/(ε2)\mathcal{O}[\varepsilon]/(\varepsilon^2). This description follows by differentiating the equations for orthogonal idempotent projections, or by writing the summands as graphs over the original summands. It uses no division by ∣H∣|H|.

For x∈Agx\in A_g and y∈Ahy\in A_h, the linearized multiplicative equations say that

δ(xy)−δ(x)y−xδ(y)(7)\delta(xy)-\delta(x)y-x\delta(y) \tag*{(7)}

has zero component in every degree other than ghgh. It also has zero ghgh-component. The first term is off degree ghgh by definition. A summand of δ(x)y\delta(x)y can have degree ghgh only if its first factor has degree gg, by cancellation in HH; that component of δ(x)\delta(x) is zero. The same reasoning applies to xδ(y)x\delta(y). Hence (7) vanishes, and δ\delta is a derivation.

The hypothesis gives δ=[a,−]\delta=[a,-] for some a∈Aa\in A. Conjugation by 1+εa1+\varepsilon a produces the specified tangent to the grading. Thus the orbit derivative from the smooth group A×A^\times is surjective onto every integral tangent module. Lemma 3.1 proves the assertion. □

Remark 3.4. The total order is fixed in Theorem 3.3. Finiteness of all crossed orders on a fixed identity order is a different assertion. For example, for odd pp the based CpC_p-crossed orders

O[t]/(tp−a),a∈O×,\mathcal{O}[t]/(t^p-a),\qquad a\in\mathcal{O}^\times,

have classes parametrized by O×/(O×)p\mathcal{O}^{\times}/(\mathcal{O}^{\times})^{p}. The principal-unit quotient is infinite: the pp-adic logarithm identifies (1+pO)/(1+pO)p(1+p\mathcal{O})/(1+p\mathcal{O})^{p} with pO/p2O≅kp\mathcal{O}/p^{2}\mathcal{O}\cong k. Their total orders vary. The crossed-product finiteness theorem in the published [7] Corollary 4.9 assumes a p′p'-grading group. Theorem 3.3 uses a different hypothesis and has just been proved also for groups divisible by pp.

From Morita classes to based graded types

For a crossed order on a fixed identity order, fixing the grading group also fixes the total rank. This converts a finite Morita list into a finite isomorphism list, to which the grading theorem applies.

Proposition 3.5 (Retaining the identity marking). Fix a basic block order RR and a finite group HH. Let A\mathcal{A} be a collection of HH-crossed orders on RR, each Morita equivalent to a finite-group block. If the total orders in A\mathcal{A} have finitely many O\mathcal{O}-Morita classes, then A\mathcal{A} has finitely many based graded isomorphism classes.

Proof. The total order. Every order in the collection has rank ∣H∣rank⁡OR|H|\operatorname{rank}_{\mathcal{O}}R. Choose a basic representative in each of its finitely many Morita classes. Any order in that class is an endomorphism order of a projective generator ⨁iPimi\bigoplus_i P_i^{m_i}, with positive integer multiplicities mim_i and the PiP_i ranging over the finitely many indecomposable projectives. Its endomorphism order contains Mmi(End⁡(Pi))M_{m_i}(\operatorname{End}(P_i)) as a direct O\mathcal{O}-module summand, so its rank bounds mi2m_i^2. There are consequently only finitely many ungraded isomorphism types in the collection.

The grading and the marking. Lemma 3.2 and Theorem 3.3 give finitely many labelled HH-gradings on every such total order. Fix one graded representative with identity component isomorphic to RR. Two identifications of that component with RR differ by an element of Aut⁡O(R)\operatorname{Aut}_{\mathcal{O}}(R). Inner changes extend to graded automorphisms of the total order by conjugation with a unit in degree one. Since Out⁡O(R)\operatorname{Out}_{\mathcal{O}}(R) is finite by Lemma 3.2, there are finitely many remaining markings. These are precisely the based graded types in the assertion. □

Teichmüller overlaps and integral Sylow comparison

The rationality bound for a Sylow restriction must compare its multiplication factors as well as its identity block. We obtain it from the explicit operators in Section 9 of [16]. Proposition 9.1 there asserts exact equivariance after reduction; here we prove exact equivariance over O\mathcal{O} by following the scalar errors through the entire integral construction. Their membership in the Teichmüller group is the point that permits the final normalization.

The scalar coefficient group

Write

T=[k×]⊆O×\mathcal{T}=[k^{\times}]\subseteq\mathcal{O}^{\times}

for the Teichmüller subgroup. Since kk is the algebraic closure of a finite field, T\mathcal{T} consists precisely of the roots of unity in O\mathcal{O} of order prime to pp. It is preserved by Witt Frobenius, which acts on it by ppth powering.

Lemma 4.1. If SS is a finite pp-group acting trivially on T\mathcal{T}, then Hi(S,T)=0H^{i}(S,\mathcal{T})=0 for every i>0i>0.

Proof. Positive-degree cohomology of a finite group is killed by its order. Raising to ∣S∣|S| is an automorphism of T\mathcal{T}, since T\mathcal{T} has no pp-torsion and has unique pp-power roots. This map also induces an automorphism on cohomology. It is simultaneously the zero map there, so the cohomology vanishes. □

Exact covariance with the prescribed factors

Proposition 4.2 (Exact integral comparison). Fix pp, MM and the data of Proposition 2.3. Let S≤Q‾S \leq\overline{Q} be a pp-subgroup contained in the pure subgroup X≤YX \leq Y, so that SS stabilizes B0=ON‾b‾B_0 = \mathcal{O}\overline{N}\overline{b}. Put as,t=ns,tb‾a_{s,t} = n_{s,t}\overline{b}. There is a positive integer mm, bounded in terms of pp, MM, and aa (σmB0,B0)(\sigma^m B_0, B_0)-Morita bimodule M\mathcal{M} with invertible O\mathcal{O}-linear maps Js:M→MJ_s : \mathcal{M} \to\mathcal{M}, normalized by J1=id⁡J_1 = \operatorname{id}, such that

Js(avb)=αs′(a)Js(v)αs(b),(8)J_s(avb) = \alpha'_s(a)J_s(v)\alpha_s(b), \tag*{(8)}
JsJt(v)=as,t′Jst(v)as,t′−1.(9)J_sJ_t(v) = a'_{s,t}J_{st}(v)a_{s,t}^{\prime-1}. \tag*{(9)}

Here a∈σmB0a \in\sigma^m B_0, b∈B0b \in B_0, αs′=σm(αs)\alpha'_s = \sigma^m(\alpha_s), and as,t′=σm(as,t)a'_{s,t} = \sigma^m(a_{s,t}). The assertion includes S=1S = 1.

The imported component operators

We first specify the integral operators that will prove Proposition 4.2. Fix its data and pure subgroup SS. The companion’s construction temporarily replaces the identity group N‾\overline{N} by a central cover. More precisely, [16], Lemma 8.2 supplies

N‾=(P×Z×∏iVi)/D0,Ji=Vi×Ci.\overline{N} = (P \times Z \times\prod_i V_i)/D_0,\qquad J_i = V_i \times C_i.

Here D0D_0 is the original central kernel, each ViV_i enlarges the universal cover of a component, and CiC_i is an added direct central pp-group. On the cross-characteristic Lie components outside the finite exceptional list, JiJ_i is the full fixed-point group of a connected reductive group with simply connected derived subgroup; on the remaining components put Ci=1C_i = 1. There is no bound on ∣D0∣|D_0| or ∣Ci∣|C_i|. The operators below are constructed on these auxiliary groups; their descent will return us to the bounded-defect block B0B_0.

Consider one SS-orbit of these Lie components. By [16], Lemmas 9.2–9.4, the product of its groups JiJ_i has a realization J=JFJ = J^F with simply connected algebraic derived subgroup and Steinberg endomorphism FF. The chosen representatives hsh_s, together with actual inner operations, generate an operation group II, represented by algebraic automorphisms commuting with FF. The source chooses a rational Levi L=LFL = L^F, a parabolic with Levi LL, and a subgroup A1A_1 of II preserving this pair, such that

I=Inn⁡(J)A1,Inn⁡(J)∩A1=Inn⁡(L),(10)I = \operatorname{Inn}(J)A_1,\qquad\operatorname{Inn}(J) \cap A_1 = \operatorname{Inn}(L), \tag*{(10)}

where A1A_1 is the particular subgroup of the cited construction. The Levi is FF-stable; its parabolic need not be. The field operations are represented by algebraic permutations with their actual relations, including the diagram twist at the cyclic wrap in the ordinary twisted realization. The exceptional graph-isogeny realization is the separate construction of that source. In particular, the representatives of SS still have the specified inner factors ns,tn_{s,t}, lifted to the central-product cover.

Let bJb_J be the lifted block and bLb_L its Levi correspondent. Set AJ=OJbJA_J = \mathcal{O}Jb_J and BL=OLbLB_L = \mathcal{O}Lb_L. The integral Bonnafé–Rouquier (AJ,BL)(A_J,B_L)-Morita bimodule UU has a strict A1A_1-action: its operators satisfy the group law exactly, and the operator for ad⁡(ℓ)\operatorname{ad}(\ell) is u↦ℓuℓ−1u \mapsto\ell u\ell^{-1} for ℓ∈L\ell\in L. Every central element of JJ acts equally from the two sides of UU [16], Lemma 9.5. Existence of the equivalence uses the full-dual-centralizer hypothesis in [4], Section 11.4, Theorem B′. Geometric comparison and extension methods are developed further in [3], Sections 6–7. The strict action used here is the companion’s action by actual automorphisms of the fixed common parabolic–Levi pair; it is not a choice of comparison maps between different parabolics.

By [16], a bounded positive exponent mm and an A1A_1-invariant linear character λm\lambda_m of LL of p′p'-order satisfy

σm(bL)=λmbL.\sigma^m(b_L)=\lambda_m b_L.

The bound is uniform in classical rank and field size, including type A where the diagonal index need not be bounded. The exponent likewise does not depend on the orders of the added central tori or the original covering kernels. Use primes for coefficient-Frobenius images. The corresponding isomorphism is

f:BL⟶BL′,gbL⟼λm(g)−1gσm(bL).f:B_L\longrightarrow B'_L,\qquad gb_L\longmapsto\lambda_m(g)^{-1}g\sigma^m(b_L).

Let TλT_\lambda be the invertible (BL′,BL)(B'_L,B_L)-bimodule with underlying left module BL′B'_L and right action through ff. Writing U∨U^\vee for a (BL,AJ)(B_L,A_J)-Morita inverse of UU, the component comparison bimodule is

MJ=σm(U)⊗BL′Tλ⊗BLU∨.(11)\mathcal{M}_J=\sigma^m(U)\otimes_{B'_L}T_\lambda\otimes_{B_L}U^\vee. \tag*{(11)}

All three factors have strict A1A_1-actions: geometric action and its dual on the outside, and the action on the group basis on the middle factor. Denote their tensor action by DaD_a. For g∈Jg\in J let Eg(v)=gvg−1E_g(v)=gvg^{-1} be the actual inner operator on MJ\mathcal{M}_J. The construction gives

EgEh=Egh,DaEgDa−1=Ea(g),(12)E_gE_h=E_{gh},\qquad D_aE_gD_a^{-1}=E_{a(g)}, \tag*{(12)}
Dad⁡(ℓ)=λm(ℓ)−1Eℓ(ℓ∈L).(13)D_{\operatorname{ad}(\ell)}=\lambda_m(\ell)^{-1}E_\ell\qquad(\ell\in L). \tag*{(13)}

The last equality is the explicit overlap calculation in the proof of [16]: on the middle factor, right multiplication uses f(ℓ−1)=λm(ℓ)ℓ−1f(\ell^{-1})=\lambda_m(\ell)\ell^{-1}. It is an equality of integral operators, not merely of their reductions.

Proof of the exact comparison

Proof of Proposition 4.24.2. The imported operators retain the actual inner factors. We show first that all their presentation ambiguities lie in T\mathcal{T}, then assemble and descend the component comparisons. Only after this descent will we remove the resulting scalar cocycle.

Teichmüller-valued presentation ambiguities. Every scalar in (13) belongs to T\mathcal{T}, because λm\lambda_m has p′p'-order. To represent an operation i∈Ii\in I, choose i=ad⁡(g)ai=\operatorname{ad}(g)a using (10) and take EgDaE_gD_a. Changing this presentation is a change through Inn⁡(L)\operatorname{Inn}(L), and hence introduces only a value of λm\lambda_m, apart from the ambiguity of a central element in the choice of gg.

That central ambiguity is also Teichmüller-valued. If c∈Z(J)c\in Z(J) is a pp-element, then c∈Lc\in L and (13) applied to it says Ec=1E_c=1: the inner operation is the identity and λm(c)=1\lambda_m(c)=1. If cc has p′p'-order, it acts on each block side by the value of its central character. The operator EcE_c is the ratio of these two p′p'-roots of unity, and lies in T\mathcal{T}. An arbitrary central element is a product of its pp- and p′p'-parts. Thus any two presentations give operators differing by T\mathcal{T}, rather than by an arbitrary unit of O\mathcal{O}.

Multiplication of chosen operators uses only (12) and a change of presentation. Its scalar discrepancy is consequently in T\mathcal{T}. Applying this to the relation αsαt=ad⁡(ns,t)αst\alpha_s\alpha_t=\operatorname{ad}(n_{s,t})\alpha_{st} shows, with the actual inner factor retained, that the resulting transport has the form

DsDt(v)=cJ(s,t)ns,t′Dst(v)ns,t′−1,cJ(s,t)∈T.D_sD_t(v)=c_J(s,t)n'_{s,t}D_{st}(v)n_{s,t}^{\prime-1},\qquad c_J(s,t)\in\mathcal{T}.

Products, component permutations and the remaining factors. We now use the remaining constructions in the proof of [16]. There are boundedly many component orbits. Taking a common bounded multiple of their exponents is legitimate by tensoring successive Frobenius twists of the comparison bimodules. Frobenius preserves T\mathcal{T}, and tensor products multiply the scalar discrepancies. This operation therefore preserves their membership in T\mathcal{T}.

For the finite list of exceptional, sporadic, and relevant defining-characteristic components, a common Frobenius period allows the identity bimodule with strict group transports. The unbounded alternating-cover family also has a uniformly bounded coefficient period, as proved in that proposition, and uses the same strict transports. The bounded pp-group factor PP uses its identity bimodule. The central p′p'-factor ZZ has a rank-one character algebra, so its left/right discrepancy is a ratio of p′p'-character values and belongs to T\mathcal{T}. Permutation of factors uses the ordinary flips of bimodules and satisfies its group relations strictly. These are tensors of ordinary Morita bimodules, so no graded symmetry sign enters this step, including when p=2p=2.

Descent through the original central kernels. It remains to pass from P×Z×∏iJiP \times Z \times\prod_i J_i to N‾\overline{N}: quotient by the added factors CiC_i and the original kernel D0D_0. The established construction identifies the left and right actions of every central pp-element on the comparison. Quotienting by c−1c-1 on the two sides therefore gives a Morita bimodule over the corresponding quotient blocks: tensor the inverse equivalence as well and use equality of the central actions in the two inverse identities. The transport maps preserve these ideals and descend. The pp-part of the quotient kernel acts trivially on both sides in the chosen averaging sector. Thus this descent introduces no new scalar factor. Differences between lifts of the prescribed ns,tn_{s,t} vanish in the quotient. In particular, the Morita equivalence and its transport maps now live on the original identity blocks, where the defect bound of Proposition [2](ii) applies.

We have obtained an integral (σmB0,B0)(\sigma^m B_0,B_0)-Morita bimodule M\mathcal{M} with O\mathcal{O}-linear covariance maps DsD_s satisfying

DsDt(v)=c(s,t)as,t′Dst(v)as,t−1,c(s,t)∈T.(14)D_sD_t(v)=c(s,t)a'_{s,t}D_{st}(v)a_{s,t}^{-1},\qquad c(s,t)\in\mathcal{T}. \tag*{(14)}

The exponent remains bounded in terms of pp, MM; the orders of the central kernels have not been bounded or used in a finiteness criterion.

Removal of the scalar error. Normalize D1=id⁡D_1=\operatorname{id}. Compare (DsDt)Dv(D_sD_t)D_v and Ds(DtDv)D_s(D_tD_v). Covariance and Equation (5) on the two block sides cancel all the non-scalar terms and leave

c(s,t)c(st,v)=c(t,v)c(s,tv).c(s,t)c(st,v)=c(t,v)c(s,tv).

Because the maps are O\mathcal{O}-linear, the scalar action is trivial. Thus cc is a normalized 2-cocycle in Z2(S,T)Z^2(S,\mathcal{T}). Lemma [4] makes it a coboundary. Rescaling each DsD_s by a normalized T\mathcal{T}-valued 1-cochain gives JsJ_s and Equation (9), without changing the covariance equation or the exponent mm.

The construction proves the scalar restriction before it uses cohomology. General O×\mathcal{O}^{\times}-valued projective transports would not suffice, since their principal-unit errors need not vanish on SS. Here Equation (11), its overlap characters and its central descent give the more precise coefficient group T\mathcal{T} at every stage.

Finite based lists on pp-subgroups

Exact comparison and fixed-total-order rigidity now meet. We first extend the comparison to a Morita equivalence of crossed orders. We then realize the relevant orders as actual blocks and apply the numerical finiteness criterion. Finally we recover the labelled components and the identity markings using Proposition [3].

Extending an exact comparison

The following is the one-term crossed-order version of the diagonal extension argument of Marcus [15], Theorem 3.4, also recorded in [18], Lemma 10.2.8. We give its algebraic proof to retain the specified multiplication factors.

Lemma 5.1 (Extension of a comparison bimodule). Let B,B′B,B' be O\mathcal{O}-orders with normalized crossed systems (αs,as,t)(\alpha_s,a_{s,t}) and (αs′,as,t′)(\alpha'_s,a'_{s,t}) for a finite group SS, and let A,A′A,A' be their crossed orders. Suppose an (B′,B)(B',B)-Morita bimodule M\mathcal{M} has invertible O\mathcal{O}-linear maps JsJ_s satisfying Equations (8) and (9). Then AA and A′A' are O\mathcal{O}-linearly Morita equivalent.

Proof. The induced right module carries the required left crossed action precisely because the comparison has the exact factor identity. Put P=M⊗BAP=\mathcal{M}\otimes_B A, a right AA-module. The left B′B'-action is the original action on M\mathcal{M}. Define right AA-linear operators

Ls(v⊗a)=Js(v)⊗usa.L_s(v\otimes a)=J_s(v)\otimes u_sa.

They are well defined on the balanced tensor product: covariance and usb=αs(b)usu_sb=\alpha_s(b)u_s identify the images of vb⊗avb\otimes a and v⊗bav\otimes ba. They are invertible, and covariance gives Lsb′=αs′(b′)LsL_sb'=\alpha'_s(b')L_s. The exact factor identity gives

LsLt(v⊗a)=as,t′Jst(v)as,t′−1⊗as,tusta=as,t′Lst(v⊗a).\begin{aligned} L_sL_t(v\otimes a)&=a'_{s,t}J_{st}(v)a_{s,t}^{\prime-1}\otimes a_{s,t}u_{st}a\\ &=a'_{s,t}L_{st}(v\otimes a). \end{aligned}

Thus these operators define a left A′A'-action.

The right BB-module M\mathcal{M} is a finitely generated projective generator. Inducing its projective summand and generator identities to AA shows that PP is a projective generator as a right AA-module. It remains to identify its endomorphism order with A′A'.

As a right BB-module, PP is the direct sum of the components M⊗BBus\mathcal{M}\otimes_B Bu_s. Induction–restriction adjunction gives the following isomorphisms of O\mathcal{O}-modules:

End⁡A(P)≅Hom⁡B(M,P)≅⨁s∈SHom⁡B(M,M⊗BBus).\operatorname{End}_A(P)\cong\operatorname{Hom}_B(\mathcal{M},P)\cong\bigoplus_{s\in S}\operatorname{Hom}_B(\mathcal{M},\mathcal{M}\otimes_B Bu_s).

Explicitly, a BB-linear map ff extends uniquely to the AA-endomorphism v⊗a↦f(v)av\otimes a\mapsto f(v)a. For a map in the degree-ss summand, composing its extension with Ls−1L_s^{-1} gives a degree-one endomorphism, hence an element of End⁡B(M)=B′\operatorname{End}_B(\mathcal{M})=B'. Therefore

End⁡A(P)=⨁s∈SB′Ls.\operatorname{End}_A(P)=\bigoplus_{s\in S}B'L_s.

The relations already checked identify this order with A′A'. The projective-generator characterization of Morita equivalence now proves the lemma.

The actual extension blocks

Proposition 5.2 (Sylow restrictions are block orders). For the data of Proposition eq:2.3, let S≤Q∩XS\leq Q\cap X be a pure pp-subgroup. The restriction of the crossed order to SS, with identity component B0B_0, is a block of a finite group. Its defect order is bounded in terms of pp, MM, and its integral Morita–Frobenius number is bounded in the same parameters. All these restriction blocks have finitely many integral Morita classes.

Proof. Constructing the group and its block. Use the actual automorphisms αs\alpha_s of N‾\overline{N} and actual elements ns,t∈Nn_{s,t} \in N supplied by Proposition 2.3(ii). On the finite set N‾×S\overline{N} \times S define

(g,s)(h,t)=(gαs(h)ns,t,st).(15)(g,s)(h,t) = (g\alpha_s(h)n_{s,t},st). \tag*{(15)}

Equations (4) and (5) give associativity, and their normalizations give the identity and inverses. Hence this is a finite group ΓS\Gamma_S with normal subgroup N‾\overline{N} and quotient SS. Sending the crossed generator usu_s to (1,s)(1,s) identifies the restriction of the unprojected crossed order with OΓS\mathcal{O}\Gamma_S.

The block b‾\overline{b} is SS-stable. A stable block has a unique covering block in an extension of pp-power index. Its idempotent is b‾\overline{b}, so our restriction is exactly

AS=OΓSb‾.A_S=\mathcal{O}\Gamma_S\overline{b}.

Bounding its defect and coefficient period. If DD is a defect group of this block, normal block theory gives a defect group D∩N‾D\cap\overline{N} of b‾\overline{b}, after conjugacy. Moreover DD maps into SS, and in this stable pp-extension it maps onto SS. In particular,

∣D∣≤∣S∣∣D∩N‾∣.|D| \leq|S||D\cap\overline{N}|.

Both quantities on the right are bounded by Proposition 2.3. Notice that the bound is applied to the group after the central descent in Section 4.

Proposition 4.2, applied to these same actual factors, and Lemma 5.1 give a Morita equivalence between ASA_S and σmAS\sigma^m A_S, with mm uniformly bounded. Thus mO(AS)≤mm_{\mathcal{O}}(A_S) \leq m. We now have an actual block with both required local bounds. Write M1(p,M)M_1(p,M) for the defect-order bound just obtained. Proposition 2.1(i), applied with M1(p,M)M_1(p,M), bounds its Cartan sum. Part (ii) of that proposition gives the claimed finite integral Morita list. There are only finitely many abstract groups SS of the possible bounded orders.

Full basic corners and arbitrary markings

Passing to a basic identity component is the integral crossed-product corner construction of [7], Proposition 4.15 and Corollary 4.16. We recall it below to retain the homogeneous units and their labels.

Theorem 5.3 (Based finiteness on pp-subgroups). Compress the crossed orders of Proposition 2.3 by a basic idempotent in the identity block, and identify the resulting identity order with a representative RiR_i of its finite list. For every possible abstract pp-group SS, their restrictions to SS have finitely many based graded isomorphism classes. The identity-order identifications may be chosen arbitrarily over O\mathcal{O}.

Proof. Pure subgroups and a fixed identity order. First suppose SS is pure. Let ee be a basic idempotent of B0B_0. For every homogeneous automorphism, its translate of ee is conjugate to ee by a unit of B0B_0: both idempotents represent a projective module containing one copy of every indecomposable projective type. Correcting each homogeneous unit by such a unit of B0B_0 makes it commute with ee. Consequently

CS=eASeC_S=eA_Se

is a crossed order on R=eB0eR=eB_0e, and

rank⁡OCS=∣S∣rank⁡OR.(16)\operatorname{rank}_{\mathcal{O}} C_S=|S|\operatorname{rank}_{\mathcal{O}} R. \tag*{(16)}

The idempotent ee is full in ASA_S, since it is already full in B0B_0.

Proposition 5.2 gives finitely many Morita classes for these total orders. For fixed RR and SS, Proposition 3.5 now gives finitely many based graded types. The proof of that proposition applies here because each CSC_S is Morita equivalent to the actual block ASA_S. In particular, its first Hochschild cohomology vanishes. (16) also displays explicitly the rank bound used to pass from Morita classes to isomorphism classes of total orders.

Transport from arbitrary subgroups. For an arbitrary pp-subgroup of QQ, conjugate by a character in Ξ\Xi to make it pure, as explained after Proposition 2.3. Conjugation is implemented by an integral homogeneous unit and transports the identity block and its full basic corner. The transported identity order is still in the same finite list. Arbitrary integral markings are already included in Proposition 3.5; inner differences are absorbed by conjugation in degree one, and outer differences form a finite set. Transporting back proves the assertion for the original subgroup and all its markings.

The information retained by this theorem is stronger than a Morita list: an isomorphism fixes the specified copy of RR and every group label. This is exactly what the kernel argument will need when it compares central factor systems after correcting the matrix actions. The integral finiteness came from actual block orders and rigidity, without a point count over W(Fq)W(\mathbb{F}_q).

Removing an unbounded prime-to-pp kernel

We now turn the finite based lists on pp-subgroups into a finite Morita list for block summands of the whole crossed order. Its grading group may have unbounded order. The bounded quantity is its index over its largest normal p′p'-subgroup.

The proof refines the field argument of [16] through the Clifford-theoretic matrix corners of [13, 14]. Over O\mathcal{O}, the principal-unit argument uses unique prime-to-pp divisibility. Removing a matrix factor creates a second scalar error; determinant normalization places it in T\mathcal{T}, so the original based Sylow restriction is recovered exactly. After these two steps, the remaining crossed systems have bounded grading groups and finite fibres under restriction.

Central units and the restriction kernel

The principal-unit argument follows [7]. Sylow restriction will control the part for which the grading group may have pp-torsion.

Lemma 6.1 (Units of the centre). Let RR be an indecomposable O\mathcal{O}-order and put ZR=Z(R)Z_R=Z(R). Then ZRZ_R is local with residue field kk, and

ZR×=T×UR,UR=1+rad⁡ZR.(17)Z_R^\times=\mathcal{T}\times U_R,\qquad U_R=1+\operatorname{rad} Z_R. \tag*{(17)}

This decomposition is invariant under every O\mathcal{O}-algebra automorphism of RR. If nn is prime to pp, the map u↦unu\mapsto u^n is an automorphism of URU_R.

Proof. The finite commutative O\mathcal{O}-algebra ZRZ_R is a product of complete local algebras, by henselianity of O\mathcal{O}. More than one factor would give a nontrivial central idempotent of RR. It is therefore local. Its residue field is a finite extension of the algebraically closed field kk, hence is kk. The residue map on units is split by the scalar Teichmüller units, and its kernel is URU_R, proving (17). Both factors are canonical and are preserved by the stated automorphisms; these act trivially on T\mathcal{T}.

For u∈URu\in U_R, the polynomial Xn−uX^n-u has the root 1 modulo the maximal ideal, with derivative nn a unit. Hensel’s lemma gives a unique root in URU_R. This proves the last assertion.

Lemma 6.2 (Finite kernel of Sylow restriction). Let a finite group QQ act by O\mathcal{O}-algebra automorphisms on ZRZ_R, and let SS be a Sylow pp-subgroup of QQ. Then

res⁡:H2(Q,ZR×)⟶H2(S,ZR×)\operatorname{res}: H^2(Q,Z_R^\times) \longrightarrow H^2(S,Z_R^\times)

has finite kernel.

Proof. The two factors in Equation (17) play different roles: restriction is injective on the principal-unit part, while the entire Teichmüller cohomology group is finite. On URU_R the composite cor⁡∘res⁡\operatorname{cor}\circ\operatorname{res} is multiplication by [Q:S][Q:S]. This is an automorphism on URU_R, by Lemma 6.1, and therefore on its cohomology. Restriction is consequently injective on H2(Q,UR)H^2(Q,U_R).

On T\mathcal{T}, the action is trivial and H2(Q,T)H^2(Q,\mathcal{T}) is finite. Indeed, let d=∣Q∣d=|Q|. The ddth-power map on T\mathcal{T} is onto and has the finite kernel μd(O)∩T\mu_d(\mathcal{O})\cap\mathcal{T}. The exact sequence in cohomology and the annihilation of positive cohomology by dd show that H2(Q,T)H^2(Q,\mathcal{T}) is a quotient of

H2(Q,μd(O)∩T),H^2(Q,\mu_d(\mathcal{O})\cap\mathcal{T}),

which is finite because both the group and the coefficient module are finite. Combining the two factors proves the lemma.

The integral extension theorem

Theorem 6.3 (Integral kernel removal). Fix an indecomposable basic O\mathcal{O}-order RR Morita equivalent to a finite-group block, and a finite subgroup F≤Out⁡O(R)\mathcal{F}\leq\operatorname{Out}_{\mathcal{O}}(R). Consider crossed orders on RR by finite groups QQ with the following properties:

  • (i) the indices [Q:Op′(Q)][Q:O_{p'}(Q)] are bounded;

  • (ii) every outer action has image in F\mathcal{F};

  • (iii) for each possible abstract pp-group, the restrictions to subgroups of that type have finitely many based graded isomorphism classes.

Then the block summands of these crossed orders have only finitely many O\mathcal{O}-linear Morita equivalence classes.

Proof. Write A=⨁q∈QRuqA=\bigoplus_{q\in Q}Ru_q for one crossed order and set

K=Op′(Q)∩ker⁡(Q⟶F).(18)K=O_{p'}(Q)\cap\ker(Q\longrightarrow\mathcal{F}). \tag*{(18)}

It is a normal p′p'-subgroup, and [Q:K]≤[Q:Op′(Q)]∣F∣[Q:K]\leq[Q:O_{p'}(Q)]|\mathcal{F}| is bounded. We isolate its twisted group algebra, pass to matrix corners, verify their Sylow restrictions, and finally count central factor systems on the bounded quotient.

Scalar factors on $K. Since KK acts trivially modulo inner automorphisms, change the KK-degree units so that they centralize RR. Their factors belong to ZR×Z_R^\times and form an ordinary 2-cocycle for the trivial KK-action. Multiplication by ∣K∣|K| is invertible on URU_R, so Hi(K,UR)=0H^i(K,U_R)=0 for i>0i>0. Removing the URU_R-component by a central change of units gives units vkv_k with

vkvl=β(k,l)vkl,β(k,l)∈T.v_kv_l=\beta(k,l)v_{kl},\qquad\beta(k,l)\in\mathcal{T}.

Their O\mathcal{O}-span is a twisted group algebra E=OβKE=\mathcal{O}_\beta K, and the restriction to KK is R⊗OER\otimes_{\mathcal{O}}E. Every homogeneous unit of AA normalizes EE. To verify this, write

uqvkuq−1=zkvqkq−1,zk∈ZR×.u_qv_ku_q^{-1}=z_kv_{qkq^{-1}},\qquad z_k\in Z_R^\times.

The coefficient is central because both sides centralize RR. Comparing the products for k,l∈Kk,l \in K shows that their URU_R-components define a homomorphism K→URK \to U_R: the original factors, their conjugates, and the factors in the new KK-degrees all lie in T\mathcal{T}. Such a homomorphism is trivial, since multiplication by ∣K∣|K| is invertible on URU_R. Hence every zkz_k belongs to T\mathcal{T}, proving normalization of EE.

The matrix factors of EE. The finitely many values of β\beta generate a finite p′p'-subgroup of T\mathcal{T}. The usual central extension defined by β\beta is therefore a finite p′p'-group, and EE is its character summand over O\mathcal{O}. A finite p′p'-group algebra over O\mathcal{O} is a product of full matrix algebras: its reduction is split semisimple, and the matrix units lift over the complete ring O\mathcal{O}. Each lifted primitive corner has rank one and is O\mathcal{O}. We obtain

E≅∏jMnj(O).(19)E \cong\prod_j M_{n_j}(\mathcal{O}). \tag*{(19)}

Every njn_j is prime to pp. Indeed these are ordinary irreducible character degrees in the indicated character sector of a finite p′p'-group; each such degree divides the group order.

Let eje_j denote the identity of one matrix factor. The QQ-orbits on these idempotents give central summands of AA. In each orbit summand a single eje_j is full, because its homogeneous conjugates sum to that orbit idempotent. Let QjprQ_j^{\mathrm{pr}} be its stabilizer. It contains KK, and the eje_j-corner, with its grading coarsened by KK, is crossed over

R⊗OMn(O),n=nj,R \otimes_{\mathcal{O}} M_n(\mathcal{O}), \qquad n=n_j,

by the group Qj=Qjpr/KQ_j=Q_j^{\mathrm{pr}}/K. The order of QjQ_j is bounded by [Q:K][Q:K].

In each QjQ_j-degree choose a unit ejuqe_j u_q inherited from an original QQ-degree. Its conjugation preserves both RR and Mn(O)M_n(\mathcal{O}), by the normalization of EE proved above. Every O\mathcal{O}-algebra automorphism of Mn(O)M_n(\mathcal{O}) is inner. For example, its images of the standard matrix idempotents split On\mathcal{O}^n into free rank-one summands; choosing compatible basis vectors for the matrix units constructs an implementing matrix. Correct the homogeneous units by these matrices so that they centralize the matrix factor. Their multiplication factors then lie in its centralizer inside R⊗OMn(O)R \otimes_{\mathcal{O}} M_n(\mathcal{O}), namely RR. The orbit corner is consequently

Mn(O)⊗OCj,M_n(\mathcal{O}) \otimes_{\mathcal{O}} C_j,

where CjC_j is a QjQ_j-crossed order on RR with the same outer action on RR. Equivalently, CjC_j is the centralizer of the matrix factor in the orbit corner.

This passage replaces the unbounded group QQ by the bounded group QjQ_j. It has not yet supplied a finite list: the matrix corrections may change the multiplication factors of a restriction. We next recover those factors. The matrix size need not be bounded; its prime-to-pp property is what the recovery uses.

Preservation of the based Sylow restriction. Let SS be a Sylow pp-subgroup of QjQ_j. Schur–Zassenhaus in its inverse image gives a pp-subgroup S~≤Qjpr\widetilde{S} \leq Q_j^{\mathrm{pr}} mapping isomorphically onto SS. Use the original units usu_s in these degrees, with original factors as,t∈R×a_{s,t} \in R^\times. Their conjugations on Ej=Mn(O)E_j=M_n(\mathcal{O}) form an honest group action, since as,ta_{s,t} centralizes EjE_j.

Choose implementing matrices cs∈GL⁡n(O)c_s \in\operatorname{GL}_n(\mathcal{O}), with c1=1c_1=1. We may take det⁡cs=1\det c_s=1. In fact, since p∤np \nmid n, every unit of O\mathcal{O} has an nnth root: take a Teichmüller root of its residue and then use Hensel’s lemma on the principal-unit part. Multiplication by a scalar thus normalizes the determinant without changing the implemented automorphism.

Because the automorphisms form a group action, there is a scalar γ(s,t)∈O×\gamma(s,t) \in\mathcal{O}^\times such that

csctcst−1=γ(s,t)In.c_s c_t c_{st}^{-1}=\gamma(s,t)I_n.

Taking determinants gives γ(s,t)n=1\gamma(s,t)^n=1. Thus γ(s,t)∈T\gamma(s,t)\in\mathcal{T}, since nn is prime to pp. Associativity shows that γ\gamma is a normalized T\mathcal{T}-valued 2-cocycle on SS.

For the corrected units ws=cs−1ejusw_s=c_s^{-1}e_j u_s, their actions on RR are unchanged. The formula for their products is

wswt=γ(s,t)−1as,twst.(20)w_sw_t=\gamma(s,t)^{-1}a_{s,t}w_{st}. \tag*{(20)}

For example, this follows by using usctus−1=csctcs−1u_sc_tu_s^{-1}=c_sc_tc_s^{-1} in the product on the left. Lemma 4.1 removes γ\gamma by scalar rescaling. Therefore the restriction of CjC_j to SS is based-isomorphic to the original restriction to S~\widetilde{S}. The corrected units generate the corresponding homogeneous RR-components of the centralizer CjC_j. For a fixed original unit, any two implementing matrices differ by a scalar unit; the subsequent scalar rescaling also changes only the generator of its component. Thus these choices change the presentation, not the based graded order. Hypothesis (iii) supplies a finite list for the restrictions now obtained.

Crossed systems on a bounded quotient. There are finitely many possible abstract groups QjQ_j and outer homomorphisms Qj→FQ_j\to F. Fix one of each and choose representatives αq∈Aut⁡O(R)\alpha_q\in\operatorname{Aut}_O(R) of its outer classes. Changing homogeneous units makes every crossed system with this outer action use these same automorphisms. If any factors satisfying the crossed identities exist, their classes under central changes of units form a torsor under

H2(Qj,ZR×).(21)H^2(Q_j,Z_R^\times). \tag*{(21)}

Indeed, the ratio of two factor systems with these fixed actions is central by Equation (1). Equation (2) says that the ratio is a 2-cocycle. A homogeneous-unit change preserving every αq\alpha_q must itself be central, and changes the ratio by a coboundary. The action on the centre is a genuine group action because inner automorphisms act trivially there.

On a Sylow pp-subgroup, the based finiteness just proved gives finitely many restricted torsor classes. To see that the fixed representatives cause no extra ambiguity, observe that a based isomorphism between systems with the same automorphisms must change their units centrally. Lemma 6.2 gives finite fibres for the restriction map from Equation (21): a nonempty fibre is a coset of its finite kernel. Thus there are finitely many based crossed orders CjC_j.

Each CjC_j has only finitely many block summands. The orbit corners above are matrix algebras over them, and the selected eje_j was full in the corresponding orbit summand of AA. Hence every block summand of AA is Morita equivalent to one of this finite list of block summands of the CjC_j. Neither the number of matrix factors in Equation (19) nor their sizes had to be bounded. This proves the theorem.

The two scalar normalizations in this proof have different reasons. On KK, its prime-to-pp order makes principal-unit cohomology vanish. On the lifted Sylow subgroup, the determinant first forces the error into T\mathcal{T}, and only its T\mathcal{T}-cohomology is used. Neither step asserts vanishing of principal-unit cohomology on a pp-group.

Proof of integral Donovan finiteness

Fix pp and MM. The previous sections supply three inputs for the last step: finitely many integral basic identity orders, finite based restrictions on their pp-subgroups, and the integral kernel-removal theorem. We check these inputs for an arbitrary finite-group block.

Proof of Theorem 1.1. Let BB be a block of OG\mathcal{O}G with defect order at most MM. Reduction and the identity order. The integral An–Eaton reduction gives a reduced pair (H,BH)(H,B_H) with BHB_H O\mathcal{O}-Morita equivalent to BB and with the same defect group. Apply Proposition 2.3. Its integral dual recovery realizes BHB_H, up to full corners, as a block summand of a crossed order on an identity block B0B_0, with grading group QQ satisfying a uniform bound on [Q:Op′(Q)][Q:O_p'(Q)].

Compress by a basic idempotent of B0B_0. As in the proof of Theorem 5.3, correction of the homogeneous units makes the resulting full corner a crossed order on one of the finite list R1,…,RtR_1,\ldots,R_t. Its outer action lies in the finite group Out⁡O(Ri)\operatorname{Out}_{\mathcal O}(R_i), by Lemma 3.2 or Proposition 2.3(iv).

The restrictions and the kernel. Theorem 5.3 supplies finitely many based restrictions on every possible pp-subgroup. Its proof used the exact integral comparison on the actual extension blocks, followed by fixed-total-order rigidity; hence these are the based restrictions required in the kernel theorem.

All three hypotheses of Theorem 6.3 now hold for this family over RiR_i: bounded [Q:Op′(Q)][Q:O_p'(Q)], finite outer-action image, and finite based pp-subgroup restrictions. Their block summands therefore have finitely many integral Morita classes.

The finite union. Taking the finite union over ii gives a list independent of GG and bb. The full-corner equivalences and the preliminary integral reduction place the original BB in that list. This proves the theorem.

Corollary 7.1. For every pp, MM, there is a finite list of integral basic orders R1′,…,Rv′R'_1,\ldots,R'_v such that the basic algebra of every block of kGkG of defect order at most MM is isomorphic to k⊗ORi′k\otimes_{\mathcal O}R'_i for some ii. In particular the blocks over kk of bounded defect have finitely many kk-linear Morita classes.

Proof. Every block idempotent over kk has its unique central idempotent lift to OG\mathcal O G. Lift a basic idempotent in that block. Its corner is an integral basic order, and reduction gives the original basic algebra. Theorem 1.1 makes the integral basic orders a finite list, proving both assertions.

The residue-field finiteness in Corollary 7.1 was already established by the field companion and supplied the Cartan input in Proposition 2.1. The corollary now identifies a finite list of integral basic orders whose reductions represent those field algebras. The proof of that stronger conclusion has used the explicit integral constructions throughout; it has not required lifting an arbitrary field Morita equivalence.

Scalar extension to a fixed complete coefficient ring

Proof of Corollary 1.2. Keep k=Fpk=\mathbb{F}_p and O=W(k)\mathcal O=W(k), and fix R\mathcal R and its residue field ℓ\ell as in the corollary. Choose an embedding ι:k↪ℓ\iota:k\hookrightarrow\ell. Since ℓ\ell is perfect, W(ℓ)W(\ell) is a Cohen ring. The coefficient-ring theorem [19] gives a local map W(ℓ)→RW(\ell)\to\mathcal R inducing the identity on ℓ\ell. It is injective: any nonzero ideal of the DVR W(ℓ)W(\ell) contains a power of pp, whereas R\mathcal R has characteristic zero. Composing with the Witt-vector map W(ℓ)W(\ell), which is injective on Witt coordinates, gives a fixed local embedding

O=W(k)→W(ι)W(ℓ)↪R\mathcal O=W(k)\xrightarrow{W(\iota)}W(\ell)\hookrightarrow\mathcal R

whose residue map is ι\iota. Only this coefficient embedding is used; no finiteness of R\mathcal R over O\mathcal O is needed.

We recall the residue-field argument of [17], Section 2.1. For every finite group GG, scalar extension identifies Z(ℓG)=ℓ⊗kZ(kG)Z(\ell G)=\ell\otimes_k Z(kG). Each local factor of the finite commutative algebra Z(kG)Z(kG) has nilpotent radical and residue field kk. After extending to ℓ\ell, the extended radical is a nilpotent ideal with quotient ℓ\ell, so the factor remains local. Consequently every primitive central idempotent bˉ\bar{b} of ℓG\ell G is uniquely of the form 1⊗bˉ01 \otimes\bar{b}_0 for a primitive central idempotent bˉ0\bar{b}_0 of kGkG. For every pp-subgroup Q≤GQ \leq G, restriction of coefficients to CG(Q)C_G(Q) gives

Br⁡Qℓ(bˉ)=1⊗Br⁡Qk(bˉ0).\operatorname{Br}^{\ell}_{Q}(\bar{b}) = 1 \otimes\operatorname{Br}^{k}_{Q}(\bar{b}_0).

Faithfulness of field extension shows that these Brauer images are nonzero for the same QQ. The characterization of defect groups as the maximal pp-subgroups with nonzero Brauer image therefore gives the same defect groups for the two residue blocks.

For either coefficient pair (Λ,F)=(O,k)(\Lambda,F) = (\mathcal{O},k) or (R,ℓ)(\mathcal{R},\ell), the class sums give a Λ\Lambda-basis of Z(ΛG)Z(\Lambda G) whose reductions give an FF-basis of Z(FG)Z(FG). Thus Z(ΛG)Z(\Lambda G) is a finite free complete commutative Λ\Lambda-algebra with residue algebra exactly Z(FG)Z(FG). Idempotents in this residue algebra lift uniquely: the derivative 2x−12x-1 of x2−xx^2-x is a unit at an idempotent modulo the maximal ideal of Λ\Lambda, so the complete-ring Hensel argument applies, including when p=2p=2. Primitivity is preserved, since central decompositions lift and an idempotent reducing to zero is zero.

Now let bb be a block idempotent of RG\mathcal{R}G, and let b0b_0 be the unique central idempotent of OG\mathcal{O}G lifting the corresponding bˉ0\bar{b}_0. The image of b0b_0 in RG\mathcal{R}G is a central idempotent reducing to bˉ\bar{b}, so uniqueness of the central lift makes it equal to bb. In particular

RGb≅R⊗O(OGb0)(22)\mathcal{R}G b \cong\mathcal{R} \otimes_{\mathcal{O}} (\mathcal{O}G b_0) \tag*{(22)}

as R\mathcal{R}-algebras, and b0b_0 has the same defect group as bb.

Finally, scalar extension preserves the specified linear Morita equivalences. Indeed, for finite O\mathcal{O}-algebras AA, BB, a O\mathcal{O}-linear Morita equivalence is represented by inverse O\mathcal{O}-central Morita bimodules BPA{}_B P_A and AQB{}_A Q_B with

P⊗AQ≅B,Q⊗BP≅A.P \otimes_A Q \cong B,\qquad Q \otimes_B P \cong A.

Write AR=R⊗OAA_{\mathcal{R}}=\mathcal{R}\otimes_{\mathcal{O}} A and similarly for BB, PP, QQ. Base change of the bimodules and their context maps gives

PR⊗ARQR≅R⊗O(P⊗AQ)≅BR,P_{\mathcal{R}} \otimes_{A_{\mathcal{R}}} Q_{\mathcal{R}} \cong\mathcal{R}\otimes_{\mathcal{O}}(P\otimes_A Q) \cong B_{\mathcal{R}},
QR⊗BRPR≅R⊗O(Q⊗BP)≅AR.Q_{\mathcal{R}} \otimes_{B_{\mathcal{R}}} P_{\mathcal{R}} \cong\mathcal{R}\otimes_{\mathcal{O}}(Q\otimes_B P) \cong A_{\mathcal{R}}.

The Morita-context identities are preserved, as are finite projectivity and the generator property. These bimodules therefore give an R\mathcal{R}-linear Morita equivalence on finitely generated modules.

Choose the finite list of O\mathcal{O}-block representatives of defect order at most MM from Theorem 1.1. The block OGb0\mathcal{O}G b_0 in (22) has that defect bound, so it is O\mathcal{O}-linearly Morita equivalent to one representative. The base-changed context puts RGb\mathcal{R}G b in the Morita class of its scalar extension. These scalar extensions form a finite list over the fixed ring R\mathcal{R}, proving the corollary.

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