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Partial Groups in Algebra and Fusion Systems

Updated 6 July 2026
  • Partial groups are algebraic structures characterized by a partially defined multiplication on words, with unit, inversion, and generalized associativity axioms.
  • They are equivalently described as reduced spiny symmetric sets, linking classical group theory to simplicial methods and fusion system frameworks.
  • The theory features a robust cohomology and extension framework alongside explicit computational classifications for finite partial groups.

Searching arXiv for recent and foundational papers on partial groups to ground the article and citations. Partial groups are algebraic structures, introduced by Chermak, in which multiplication is assigned not to all finite words in a set but only to a specified domain of words, while still satisfying unit, inversion, and generalized associativity axioms. In contemporary treatments they are equally described as reduced spiny symmetric sets, so the subject sits simultaneously in algebra, simplicial theory, and the theory of fusion systems and localities (Chermak, 2015, Hackney et al., 2023, Hackney et al., 2024).

1. Algebraic definition and immediate structure

In Chermak’s formulation, a partial group consists of a nonempty set MM, a subset DW(M)D\subseteq W(M) of the free monoid on MM, a product map Π:DM\Pi:D\to M, and an involutory bijection xx1x\mapsto x^{-1}, extended to words by reversal, such that MDM\subseteq D, uvDu,vDu\circ v\in D\Rightarrow u,v\in D, Π\Pi restricts to the identity on one-letter words, and whenever uvwDu\circ v\circ w\in D, one has uΠ(v)wDu\circ \Pi(v)\circ w\in D together with

DW(M)D\subseteq W(M)0

If DW(M)D\subseteq W(M)1, then DW(M)D\subseteq W(M)2 and DW(M)D\subseteq W(M)3, where DW(M)D\subseteq W(M)4. A group is precisely a partial group with total domain DW(M)D\subseteq W(M)5 (Chermak, 2015).

This formulation encodes a partially defined multiplication on words of arbitrary length rather than merely a partially defined binary law. Basic constructions already resemble ordinary group theory. For DW(M)D\subseteq W(M)6, the domain of conjugation by DW(M)D\subseteq W(M)7 is

DW(M)D\subseteq W(M)8

and for DW(M)D\subseteq W(M)9 one defines

MM0

A nonempty subset MM1 is a partial subgroup if it is closed under inversion and under products of words in MM2. A partial subgroup MM3 is partial normal if MM4, MM5, and MM6 imply MM7 (Chermak, 2015).

Chermak further isolates objective partial groups and localities. An objective partial group MM8 is one whose domain is determined by chains of conjugations among a specified family MM9 of subgroups. A locality Π:DM\Pi:D\to M0 is a finite objective partial group equipped with a distinguished Π:DM\Pi:D\to M1-subgroup Π:DM\Pi:D\to M2, maximal among Π:DM\Pi:D\to M3-subgroups of Π:DM\Pi:D\to M4. This is the framework in which partial groups became central in the study of fusion systems and transporter systems (Chermak, 2015).

2. Simplicial and symmetric-set formulations

A decisive reformulation identifies partial groups with special symmetric simplicial objects. A symmetric set is a presheaf on finite ordinals and all set maps between them. Such a symmetric set is spiny when its spine maps are injective; in the reduced case, meaning a single Π:DM\Pi:D\to M5-simplex, reduced spiny symmetric sets are equivalent to partial groups, while spiny symmetric sets without reduction are equivalent to partial groupoids (Hackney et al., 2023).

This viewpoint packages admissible words as simplices. If Π:DM\Pi:D\to M6 is the symmetric set associated to a partial group, then Π:DM\Pi:D\to M7 is the underlying set of elements, and an Π:DM\Pi:D\to M8-simplex corresponds to an admissible Π:DM\Pi:D\to M9-word. The injectivity of the relevant Segal-type maps means that a simplex is uniquely determined by its edges. In matrix language, an xx1x\mapsto x^{-1}0-simplex xx1x\mapsto x^{-1}1 determines entries xx1x\mapsto x^{-1}2, and for spiny symmetric sets the assignment

xx1x\mapsto x^{-1}3

is injective. This matrix picture is used throughout the modern theory to encode partial composition and inversion (Hackney et al., 2024).

The same formalism sharply separates groups and groupoids from their partial analogues. A symmetric set is isomorphic to the nerve of a groupoid exactly when the spine maps are bijections rather than merely injections. Thus partial groupoids are obtained by weakening the Segal-type bijectivity conditions to injectivity, and partial groups are the one-object case of that weakening (Hackney et al., 2024).

The symmetric-set model also clarifies categorical behavior. The category of spiny symmetric sets is reflective in the category of symmetric sets, and the category of reduced spiny symmetric sets is reflective in reduced symmetric sets. As a consequence, partial groupoids and partial groups are complete and cocomplete; limits are inherited from symmetric sets, while colimits are computed in symmetric sets and then reflected back to the spiny, reduced subcategory (Hackney et al., 2023).

3. Dimension, skeleta, and finiteness

Because symmetric sets admit a robust notion of degeneracy, partial groups carry a natural dimension theory. An element xx1x\mapsto x^{-1}4 is degenerate if it factors through a noninvertible surjection xx1x\mapsto x^{-1}5 with xx1x\mapsto x^{-1}6. The xx1x\mapsto x^{-1}7-skeleton xx1x\mapsto x^{-1}8 is the smallest symmetric subset containing all simplices of degree at most xx1x\mapsto x^{-1}9. One says that MDM\subseteq D0 is MDM\subseteq D1-skeletal if MDM\subseteq D2, and that MDM\subseteq D3 has dimension MDM\subseteq D4 if it is MDM\subseteq D5-skeletal but not MDM\subseteq D6-skeletal (Hackney et al., 2024).

For finite partial groups this dimension is tightly controlled by cardinality. If MDM\subseteq D7 is a partial group with MDM\subseteq D8 elements, regarded as a symmetric set, then MDM\subseteq D9 is uvDu,vDu\circ v\in D\Rightarrow u,v\in D0-skeletal. If uvDu,vDu\circ v\in D\Rightarrow u,v\in D1 is actually a group, then its dimension is exactly uvDu,vDu\circ v\in D\Rightarrow u,v\in D2. More generally, for a connected partial groupoid uvDu,vDu\circ v\in D\Rightarrow u,v\in D3, if the dimension reaches the maximal value allowed by the number of outgoing nonidentity arrows, then uvDu,vDu\circ v\in D\Rightarrow u,v\in D4 is already a genuine groupoid. In the one-object case this yields the rigidity statement that maximal possible dimension characterizes groups among partial groups of a given finite size (Hackney et al., 2024).

This has a strong finiteness consequence. Chermak’s original definition uses a subset uvDu,vDu\circ v\in D\Rightarrow u,v\in D5 of an infinite free monoid, so a finite underlying set can still appear to require infinitely much data. The symmetric-set description shows that this is illusory for finite partial groups: once uvDu,vDu\circ v\in D\Rightarrow u,v\in D6, all simplices above degree uvDu,vDu\circ v\in D\Rightarrow u,v\in D7 are degenerate, so the entire structure is determined by finitely many low-dimensional simplices. In particular, finite partial groups have only finitely many im-partial subgroups, meaning nonempty symmetric subsets, and there are only finitely many partial groups up to isomorphism for a fixed finite cardinality (Hackney et al., 2024).

The same dimension theory behaves differently from ordinary simplicial dimension. A finite group uvDu,vDu\circ v\in D\Rightarrow u,v\in D8 has infinitely many nonempty simplices in its usual simplicial nerve, but when regarded as a symmetric set its dimension is finite, namely uvDu,vDu\circ v\in D\Rightarrow u,v\in D9. This distinction is one of the conceptual payoffs of the symmetric-set formulation (Hackney et al., 2024).

4. Subgroups, quotients, free objects, and embeddability

The category Π\Pi0 of partial groups admits kernels, cokernels, limits, and colimits. In Salati’s formulation, one distinguishes impartial subgroups, which are precisely images of morphisms in the categorical sense, from partial subgroups, which carry the maximal induced domain. Quotients are defined as cokernels in Π\Pi1, and this construction agrees with ordinary group quotients when the partial group is a group and with Chermak’s quotient of a locality by a partial normal subgroup in the locality setting (Salati, 2021).

The same paper constructs free partial groups. There is a free partial group on a pointed set, and a richer free construction over a category of structured sets that remembers an intended domain of words and an involution. This richer notion yields a generators-and-relations theorem: every partial group is a quotient of a free partial group. In that sense partial groups admit a presentation theory analogous to the classical statement that every group is a quotient of a free group (Salati, 2021).

Embeddability into genuine groups is subtler. A folklore theorem, recorded and extended in a many-object form, states that a partial group embeds in a group if and only if each word has at most one possible multiplication, regardless of choice of parenthesization. Equivalently, all words are “kind” rather than “mean,” in the language of the paper. For partial groupoids, embeddability in a groupoid is equivalent to embeddability of the reduction in a group. The embeddable partial groups and partial groupoids form reflective subcategories, so each partial object has a universal embeddable reflection (Hackney et al., 27 Jan 2026).

At the level of elementary algebra, the category also supports homological analogues of kernels and images. Quotienting by a partial normal subgroup behaves as expected, but the embeddability criterion shows that not every partial group is merely a partial subgroup of some ambient group; ambiguity of word multiplication is the exact obstruction (Hackney et al., 27 Jan 2026).

The modern notion of partial group subsumes older partially defined group-like structures. Stallings’ pregroups admit a canonical embedding into Chermak partial groups: the category of pregroups is a full subcategory of the category of partial groups. For a pregroup Π\Pi2, the associated universal group Π\Pi3 is canonically isomorphic to the fundamental group Π\Pi4 of the simplicial classifying space of the corresponding partial group. This identifies pregroups as a combinatorial subclass of partial groups particularly well adapted to graphs of groups and amalgam-type constructions (Lemoine et al., 2023).

This comparison has consequences for fusion systems. The same work proves that every fusion system on a finite Π\Pi5-group is realizable as the fusion system of some finite pregroup, and that for a Sylow Π\Pi6-subgroup Π\Pi7 the fusion systems Π\Pi8 and Π\Pi9 coincide. This places pregroups and partial groups in the same realizability landscape, though localities remain a much more restrictive class (Lemoine et al., 2023).

A second comparison concerns binary partial groups, meaning unital partial magmas with a partially defined binary product and inverse map satisfying strong cancellation axioms. Many classical examples of “binary” partial groups in the literature turn out to lie inside Chermak’s framework. There is a fully faithful functor from binary partial groups to Chermak partial groups, and the category of binary partial groups is equivalent to the category of uvwDu\circ v\circ w\in D0-skeletal partial groups. Thus the one- and two-dimensional simplicial data already recover exactly the largest class of binary partial groups that can be canonically regarded as partial groups in Chermak’s sense (Hackney et al., 3 Mar 2026).

These comparison theorems sharpen the conceptual position of partial groups. They are broader than pregroups and binary partial magmas, but low-dimensional truncations recover those older notions exactly when the relevant coherence conditions are present (Lemoine et al., 2023, Hackney et al., 3 Mar 2026).

6. Cohomology and extension theory

A systematic cohomology theory for partial groups can be formulated in two parallel ways. Algebraically, if a partial group uvwDu\circ v\circ w\in D1 acts on an abelian group uvwDu\circ v\circ w\in D2 via a homomorphism uvwDu\circ v\circ w\in D3, one sets

uvwDu\circ v\circ w\in D4

and defines

uvwDu\circ v\circ w\in D5

These coboundaries satisfy uvwDu\circ v\circ w\in D6, giving cohomology groups uvwDu\circ v\circ w\in D7. Simplicially, one can instead take cohomology of the reduced simplicial set underlying uvwDu\circ v\circ w\in D8 with coefficients in a local system uvwDu\circ v\circ w\in D9. The two constructions coincide: uΠ(v)wDu\circ \Pi(v)\circ w\in D0 This extends ordinary group cohomology, since for uΠ(v)wDu\circ \Pi(v)\circ w\in D1 one recovers the classical bar complex and classical uΠ(v)wDu\circ \Pi(v)\circ w\in D2 (Pfammatter, 5 Dec 2025).

The main application is extension theory. An extension of a partial group uΠ(v)wDu\circ \Pi(v)\circ w\in D3 by a partial group uΠ(v)wDu\circ \Pi(v)\circ w\in D4 is a fibre bundle of simplicial sets uΠ(v)wDu\circ \Pi(v)\circ w\in D5 whose total space is again a partial group. Such extensions are encoded by twisting pairs uΠ(v)wDu\circ \Pi(v)\circ w\in D6, where uΠ(v)wDu\circ \Pi(v)\circ w\in D7 and uΠ(v)wDu\circ \Pi(v)\circ w\in D8 satisfy a cocycle condition. Fixing an outer action uΠ(v)wDu\circ \Pi(v)\circ w\in D9, one obtains an obstruction class

DW(M)D\subseteq W(M)00

An extension with outer action DW(M)D\subseteq W(M)01 exists exactly when this class vanishes, and when it does, the set of equivalence classes of extensions is a principal homogeneous space for

DW(M)D\subseteq W(M)02

For groups this specializes to the Eilenberg–MacLane classification of group extensions (Pfammatter, 5 Dec 2025).

The theory also yields explicit enumerative results. If DW(M)D\subseteq W(M)03 and DW(M)D\subseteq W(M)04 are finite pointed sets with free partial groups DW(M)D\subseteq W(M)05 and DW(M)D\subseteq W(M)06, then the number of equivalence classes of extensions of DW(M)D\subseteq W(M)07 by DW(M)D\subseteq W(M)08 is

DW(M)D\subseteq W(M)09

This contrasts sharply with free groups, whose extension theory is typically infinite (Pfammatter, 5 Dec 2025).

7. Localities, examples, and the computational landscape

Partial groups were introduced to recast transporter and fusion-theoretic structures in more group-like terms. In Chermak’s locality theory, finite localities carry distinguished DW(M)D\subseteq W(M)10-subgroups and object sets controlling which words are defined, normalizers of objects are honest groups, and quotients by partial normal subgroups preserve the locality structure. This places partial groups at the algebraic core of one of the main approaches to saturated fusion systems (Chermak, 2015).

The theory also supports more combinatorial constructions. For every simple graph DW(M)D\subseteq W(M)11, there is a path partial group DW(M)D\subseteq W(M)12 whose automorphism group satisfies

DW(M)D\subseteq W(M)13

Consequently, for any abstract group DW(M)D\subseteq W(M)14 there exist infinitely many nonisomorphic partial groups DW(M)D\subseteq W(M)15 with

DW(M)D\subseteq W(M)16

This universality phenomenon has no analogue for ordinary groups and shows that partial groups are flexible enough to encode arbitrary prescribed automorphism groups (Ramos et al., 2021).

A different line of work studies finite partial groups by exhaustive computation. There are DW(M)D\subseteq W(M)17 partial groups of order at most DW(M)D\subseteq W(M)18 and DW(M)D\subseteq W(M)19 partial groups of order DW(M)D\subseteq W(M)20. The same program gives a complete list of indecomposable partial groups of order at most DW(M)D\subseteq W(M)21, and proves structural results first observed experimentally, including the characterization of indecomposable partial groups of order DW(M)D\subseteq W(M)22 and dimension DW(M)D\subseteq W(M)23 as DW(M)D\subseteq W(M)24 for a unique group DW(M)D\subseteq W(M)25, and the theorem that a spiny symmetric set of degree at most DW(M)D\subseteq W(M)26 is DW(M)D\subseteq W(M)27-coskeletal (Hackney, 25 May 2026).

Taken together, these developments show that partial groups form a broad algebraic class with several simultaneous faces: they are generalized groups defined by partial word multiplication, reduced spiny symmetric sets, algebraic models for localities and fusion data, receptacles for pregroups and binary partial groups, and objects with a genuine cohomology and extension theory. The subject now includes structural rigidity results, categorical generators-and-relations techniques, embeddability criteria, explicit universal constructions, and large-scale computational classification (Hackney et al., 2023, Hackney et al., 2024, Pfammatter, 5 Dec 2025).

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