Papers
Topics
Authors
Recent
Search
2000 character limit reached

Separated Graph Inverse Semigroup Overview

Updated 19 December 2025
  • Separated graph inverse semigroups are universal inverse semigroups associated with separated graphs, extending classical graph theories by incorporating separation data.
  • Their detailed idempotent structure and C-compatible trees yield explicit normal forms and enable restricted semidirect product decompositions via partial actions of free groups.
  • Applications include canonical K-bases for Leavitt path algebras and C*-algebras, linking these structures to type semigroups and graph monoids.

A separated graph inverse semigroup is a universal inverse semigroup S(E,C)\mathcal{S}(E,C) associated to a separated graph (E,C)(E, C), designed to generalize the classical graph inverse semigroup theory to capture the additional combinatorics and symmetries introduced by separation data. This structure is foundational in inverse semigroup approaches to tame graph algebras, Leavitt path algebras, and CC^*-algebraic counterparts. The theory develops through detailed analysis of the idempotent structure via CC-compatible trees, semidirect product decompositions involving partial actions of free groups, and connections with the tight groupoid and type semigroups, enabling explicit normal forms and canonical algebraic bases (Ara et al., 17 Dec 2025, Ara et al., 2024, Ara et al., 2019).

1. Separated Graphs and the Inverse Semigroup S(E,C)\mathcal{S}(E,C)

A separated graph is a pair (E,C)(E, C), where E=(E0,E1,s,r)E=(E^0, E^1, s, r) is a directed graph with vertex set E0E^0 and edge set E1E^1, and C=vE0CvC=\bigsqcup_{v\in E^0} C_v is a partition of the outgoing edges at each vertex: CvC_v is a collection of pairwise disjoint, nonempty subsets partitioning s1(v)s^{-1}(v). Extremal cases include the trivial (unseparated) case where Cv={s1(v)}C_v = \{ s^{-1}(v)\} for each vv and the free separation with Cv={{e}:es1(v)}C_v = \{ \{e\} : e \in s^{-1}(v)\}.

The separated graph inverse semigroup S(E,C)\mathcal{S}(E,C) is universally generated by E0E^0, E1E^1, and their formal inverses E11E^{1-1} (with involution ee1e\mapsto e^{-1}, extended to paths), modulo the relations:

  • vw=δv,wvv w = \delta_{v, w} v for v,wE0v, w \in E^0
  • s(x)x=x=xr(x)s(x) x = x = x r(x) for xE1E11x \in E^1 \cup E^{1-1}
  • e1f=δe,fr(e)e^{-1} f = \delta_{e,f} r(e) for e,fX,XCe, f \in X, X\in C
  • xx1x x^{-1} and yy1y y^{-1} commute for all x,yS(E,C)x, y \in \mathcal{S}(E,C).

Each eE1e\in E^1 acts as a canonical partial isometry. This semigroup always contains zero $0$ and features a rich lattice of idempotents.

2. Idempotent Structure and CC-Compatible Trees

Every element of S(E,C)\mathcal{S}(E,C) can be uniquely written in Scheiblich normal form as αβ1\alpha \beta^{-1}, with α,β\alpha, \beta reduced CC-separated paths in the double graph E^\widehat E (i.e., no subword x1yx^{-1}y with x,yXx, y\in X for some XCX\in C). Idempotents are elements of the form αα1\alpha \alpha^{-1}.

The semilattice of idempotents E(S(E,C))E(\mathcal{S}(E,C)) is in bijection with the family YY of all nonempty finite CC-compatible EE-trees—finite lower sets of CC-separated paths at a base vertex, subject to compatibility (maximal path geodesic joins remain CC-separated). For such a tree TT:

e(T)=λmax(T)λλ1e(T) = \prod_{\lambda\in\max(T)} \lambda \lambda^{-1}

Idempotents are partially ordered by inclusion of their associated trees: e(T)e(T)e(T)\leq e(T') iff TTT\supseteq T'. This combinatorial structure encodes the underlying CC-separation and is central to understanding both the inverse semigroup and associated algebras (Ara et al., 17 Dec 2025, Ara et al., 2024).

3. Strong EE^*-Unitarity and (Restricted) Semidirect Product Decomposition

A defining structural result is that S(E,C)\mathcal{S}(E,C) is strongly EE^*-unitary. There exists an idempotent-pure partial homomorphism

σ:S(E,C)×F(E1)\sigma: \mathcal{S}(E,C)^\times \to \mathbb{F}(E^1)

with σ(v)=1\sigma(v)=1, σ(e)=e\sigma(e)=e, σ(e1)=e1\sigma(e^{-1})=e^{-1} (eE1e\in E^1), so that the kernel of σ\sigma is the set of idempotents. This enables a presentation of S(E,C)\mathcal{S}(E,C) as a restricted semidirect product

S(E,C)YθF\mathcal{S}(E,C) \cong \mathcal{Y} \rtimes_\theta \mathbb{F}

where F=F(E1)\mathbb{F} = \mathbb{F}(E^1) is the free group on E1E^1 and Y\mathcal{Y} is a quotient semilattice of finite CC-compatible lower sets of paths. The partial action θ\theta reflects pre- and post-concatenation dynamics, and the product is

(I,g)(J,h)=(Iθg(J),gh)(I, g)\cdot (J, h) = (I \wedge \theta_g(J),\, gh)

with inversion (I,g)1=(θg1(I),g1)(I, g)^{-1} = (\theta_{g^{-1}}(I),\, g^{-1}), restricted to cases where domains are defined (Ara et al., 2024).

4. The Leavitt Inverse Semigroup and Quotient Structures

The Leavitt inverse semigroup LI(E,C)\mathcal{LI}(E,C) is a quotient of S(E,C)\mathcal{S}(E,C) imposing the so-called single-edge Cuntz–Krieger relations ee1=s(e)ee^{-1} = s(e) whenever {e}C\{e\}\in C. Algebraically, the associated tame Leavitt path algebra LKab(E,C)\mathcal{L}_K^{\mathrm{ab}}(E,C) is obtained from the tame Cohn algebra CKab(E,C)\mathcal{C}_K^{\mathrm{ab}}(E,C) by factoring out elements qX=veXee1q_X = v-\sum_{e\in X} ee^{-1}.

A central theorem is that LI(E,C)\mathcal{LI}(E,C) remains strongly EE^*-unitary and admits a restricted semidirect product decomposition:

LI(E,C)ELrF\mathcal{LI}(E,C) \cong \mathcal{E}^L \rtimes^r \mathbb{F}

with EL\mathcal{E}^L a suitable quotient semilattice and with canonical normal forms: every element (T,g)(T, g), with TT a Leavitt–Munn tree and gg a CC-separated group element with left-special prefix in TT (Ara et al., 17 Dec 2025). This yields a linear basis for LKab(E,C)\mathcal{L}_K^{\mathrm{ab}}(E,C) via pairs (e(T),g)(e(T), g), subject to reductions along finite CC-edges.

5. Spectrum, Tight Groupoid, and Amenability

The spectrum of the semilattice of idempotents Y\mathcal{Y}, Y^\widehat{\mathcal{Y}}, is comprised of nonzero characters, identified with filters, and equipped with a totally disconnected topology. The tight spectrum Y^tight\widehat{\mathcal{Y}}_{\mathrm{tight}} is the closure of ultrafilters, corresponding concretely to infinite CC-separated paths in E^\widehat{E} and vertices with infinite emission.

The universal groupoid G(S(E,C))Y^θF\mathcal{G}(\mathcal{S}(E,C)) \cong \widehat{\mathcal{Y}} \rtimes_\theta \mathbb{F} restricts to the tight groupoid Gtight(S(E,C))Y^tightθF\mathcal{G}_{\mathrm{tight}}(\mathcal{S}(E,C)) \cong \widehat{\mathcal{Y}}_{\mathrm{tight}} \rtimes_\theta \mathbb{F} (Ara et al., 2024). For adaptable separated graphs, this groupoid is always Hausdorff, ample, and étale. Furthermore, it is amenable: the relevant examples reduce—over regular primes—to classical, amenable graph groupoids, and—over free primes—to transformation groupoids of abelian groups acting on Cantor-type spaces (Ara et al., 2019). This ensures that associated Steinberg and CC^*-algebras are nuclear and satisfy the UCT.

6. Applications to Algebras and Type Semigroups

The combinatorial normal forms arising from the structure of S(E,C)\mathcal{S}(E,C) and its quotient LI(E,C)\mathcal{LI}(E,C) yield canonical KK-bases for tame Cohn and Leavitt path algebras, generalizing the well-known Zelmanov–Alahmadi bases in the unseparated case (Ara et al., 17 Dec 2025). Under mild assumptions (adaptability), the type semigroup Typ(Gtight(S(E,C)))\mathrm{Typ}(\mathcal{G}_{\mathrm{tight}}(\mathcal{S}(E,C))) is isomorphic to the graph monoid M(E,C)M(E, C):

M(E,C)=av (vE0)  av=eXar(e), XCvM(E, C) = \langle a_v\ (v\in E^0)\ |\ a_v = \sum_{e\in X} a_{r(e)},\ X\in C_v \rangle

Every finitely generated conical refinement monoid arises this way. The direct connection to the realization problem for von Neumann regular rings and classification theory for Leavitt path algebras is a major motivation for the study (Ara et al., 2019).

Examples include:

  • Ordinary graphs (CvC_v trivial): recovers the classical theory.
  • Cuntz separated graphs (free separation): LI(E,C)\mathcal{LI}(E,C) is a free group, idempotent semilattice is trivial.
  • Realization of the free inverse monoid as a corner of a suitable separated graph inverse semigroup.
  • Computation of the socle and isolated points of the spectrum, with a splitting as direct sums of full matrix algebras over KK for the tame Leavitt algebra.

7. Illustrative Examples and Further Directions

Several explicit constructions illustrate the theory:

  • Zelmanov–Alahmadi basis: arises for the unseparated case and is recovered as a special case of the normal forms.
  • Cuntz separated graphs: demonstrate how all idempotents can collapse, leaving the free group and group algebra structure.
  • Two-fold refinement monoid: provides an example where separated graph monoids extend the range beyond classical row-finite graph monoids (Ara et al., 2019).
  • Socle and kernel computations: normal-form bases describe both the socle of Leavitt path algebras and kernels of natural maps between associated tame algebras.

The unified framework of separated graph inverse semigroups and their quotients by Leavitt-type relations enables a canonical handling of tame Cohn and Leavitt algebras and their CC^*-analogues, clarifies semidirect product decompositions, and supports combinatorial and spectral analysis essential to both algebraic and operator-algebraic applications (Ara et al., 17 Dec 2025, Ara et al., 2024).

Definition Search Book Streamline Icon: https://streamlinehq.com
References (3)

Topic to Video (Beta)

No one has generated a video about this topic yet.

Whiteboard

No one has generated a whiteboard explanation for this topic yet.

Follow Topic

Get notified by email when new papers are published related to Separated Graph Inverse Semigroup.