<p>In this paper we introduce an inverse semigroup <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {S}(E,C)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">S</mi> <mo stretchy="false">(</mo> <mi>E</mi> <mo>,</mo> <mi>C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> associated to a separated graph (<i>E</i>,&#xa0;<i>C</i>) and describe its internal structure. In particular we show that it is strongly <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(E^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>E</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>-unitary and can be realized as a partial semidirect product of the form <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq3.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {Y}\rtimes \mathbb {F}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">Y</mi> <mo>⋊</mo> <mi mathvariant="double-struck">F</mi> </mrow> </math></EquationSource> </InlineEquation> for a certain partial action of the free group <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="76" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {F}=\mathbb {F}(E^1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="double-struck">F</mi> <mo>=</mo> <mi mathvariant="double-struck">F</mi> <mo stretchy="false">(</mo> <msup> <mi>E</mi> <mn>1</mn> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> on the edges of <i>E</i> on a semilattice <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq5.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {Y}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">Y</mi> </math></EquationSource> </InlineEquation> realizing the idempotents of <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {S}(E,C)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">S</mi> <mo stretchy="false">(</mo> <mi>E</mi> <mo>,</mo> <mi>C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. In addition we also describe the spectrum as well as the tight spectrum of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq5.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {Y}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">Y</mi> </math></EquationSource> </InlineEquation>. We then use the inverse semigroup <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {S}(E,C)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">S</mi> <mo stretchy="false">(</mo> <mi>E</mi> <mo>,</mo> <mi>C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> to describe several “tame” algebras associated to (<i>E</i>,&#xa0;<i>C</i>), including its Cohn algebra, its Leavitt-path algebra, and analogues in the realm of <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="MediaObjects/574_2025_462_Figa_HTML.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="120" Type="Linedraw" Width="29" /> </InlineMediaObject>algebras, like the tame <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="MediaObjects/574_2025_462_Figb_HTML.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="120" Type="Linedraw" Width="29" /> </InlineMediaObject>algebra <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="62" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {O}}(E,C)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">O</mi> <mo stretchy="false">(</mo> <mi>E</mi> <mo>,</mo> <mi>C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and its Toeplitz extension <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq10.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="62" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {T}(E,C)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">T</mi> <mo stretchy="false">(</mo> <mi>E</mi> <mo>,</mo> <mi>C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, proving that these algebras are canonically isomorphic to certain algebras attached to <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {S}(E,C)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">S</mi> <mo stretchy="false">(</mo> <mi>E</mi> <mo>,</mo> <mi>C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. Our structural results on <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="574_2025_462_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {S}(E,C)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">S</mi> <mo stretchy="false">(</mo> <mi>E</mi> <mo>,</mo> <mi>C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> imply that these algebras can be realized as partial crossed products, revealing a great portion of their structure.</p>

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Inverse Semigroups of Separated Graphs and Associated Algebras

  • Pere Ara,
  • Alcides Buss,
  • Ado Dalla Costa

摘要

In this paper we introduce an inverse semigroup \(\mathcal {S}(E,C)\) S ( E , C ) associated to a separated graph (EC) and describe its internal structure. In particular we show that it is strongly \(E^*\) E -unitary and can be realized as a partial semidirect product of the form \(\mathcal {Y}\rtimes \mathbb {F}\) Y F for a certain partial action of the free group \(\mathbb {F}=\mathbb {F}(E^1)\) F = F ( E 1 ) on the edges of E on a semilattice \(\mathcal {Y}\) Y realizing the idempotents of \(\mathcal {S}(E,C)\) S ( E , C ) . In addition we also describe the spectrum as well as the tight spectrum of \(\mathcal {Y}\) Y . We then use the inverse semigroup \(\mathcal {S}(E,C)\) S ( E , C ) to describe several “tame” algebras associated to (EC), including its Cohn algebra, its Leavitt-path algebra, and analogues in the realm of algebras, like the tame algebra \({\mathcal {O}}(E,C)\) O ( E , C ) and its Toeplitz extension \(\mathcal {T}(E,C)\) T ( E , C ) , proving that these algebras are canonically isomorphic to certain algebras attached to \(\mathcal {S}(E,C)\) S ( E , C ) . Our structural results on \(\mathcal {S}(E,C)\) S ( E , C ) imply that these algebras can be realized as partial crossed products, revealing a great portion of their structure.