<p>We prove a version of Gabriel’s theorem for (possibly infinite dimensional) representations of infinite quivers. More precisely, we show that the representation theory of a quiver <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{\Omega }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold">Ω</mi> </mrow> </math></EquationSource> </InlineEquation> is of unique type (each dimension vector has at most one associated indecomposable) and infinite Krull-Schmidt (every, possibly infinite dimensional, representation is a direct sum of indecomposables) if and only if <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{\Omega }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold">Ω</mi> </mrow> </math></EquationSource> </InlineEquation> is eventually outward and of generalized ADE Dynkin type (<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="27" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{A_n}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="bold-italic">A</mi> <mi mathvariant="bold-italic">n</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{D_n}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="bold-italic">D</mi> <mi mathvariant="bold-italic">n</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{E_6}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="bold-italic">E</mi> <mn mathvariant="bold">6</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{E_7}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="bold-italic">E</mi> <mn mathvariant="bold">7</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{E_8}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="bold-italic">E</mi> <mn mathvariant="bold">8</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq8.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{A_\infty }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="bold-italic">A</mi> <mi mathvariant="bold-italic">∞</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{A_{\infty , \infty }}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="bold-italic">A</mi> <mrow> <mi mathvariant="bold-italic">∞</mi> <mo mathvariant="bold">,</mo> <mi mathvariant="bold-italic">∞</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>, or <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{D_\infty }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="bold-italic">D</mi> <mi mathvariant="bold-italic">∞</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>). Furthermore we define an analog of the Euler-Tits form on the space of eventually constant infinite roots and show that a quiver is of generalized ADE Dynkin type if and only if this form is positive definite. In this case the indecomposables are all locally finite-dimensional and eventually constant and correspond bijectively to the positive roots (i.e. those of length <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10468_2025_10349_Article_IEq11.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varvec{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn mathvariant="bold">1</mn> </mrow> </math></EquationSource> </InlineEquation>).</p>

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Gabriel’s Theorem for Infinite Quivers

  • Nathaniel Gallup,
  • Stephen Sawin

摘要

We prove a version of Gabriel’s theorem for (possibly infinite dimensional) representations of infinite quivers. More precisely, we show that the representation theory of a quiver \(\varvec{\Omega }\) Ω is of unique type (each dimension vector has at most one associated indecomposable) and infinite Krull-Schmidt (every, possibly infinite dimensional, representation is a direct sum of indecomposables) if and only if \(\varvec{\Omega }\) Ω is eventually outward and of generalized ADE Dynkin type ( \(\varvec{A_n}\) A n , \(\varvec{D_n}\) D n , \(\varvec{E_6}\) E 6 , \(\varvec{E_7}\) E 7 , \(\varvec{E_8}\) E 8 , \(\varvec{A_\infty }\) A , \(\varvec{A_{\infty , \infty }}\) A , , or \(\varvec{D_\infty }\) D ). Furthermore we define an analog of the Euler-Tits form on the space of eventually constant infinite roots and show that a quiver is of generalized ADE Dynkin type if and only if this form is positive definite. In this case the indecomposables are all locally finite-dimensional and eventually constant and correspond bijectively to the positive roots (i.e. those of length \(\varvec{1}\) 1 ).