<p>The tridiagonal algebra is defined by two generators and two relations, called the tridiagonal relations. Special cases of the tridiagonal algebra include the <i>q</i>-Onsager algebra, the positive part of the <i>q</i>-deformed enveloping algebra <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10801_2025_1420_Article_IEq3.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\(U_q({\widehat{\mathfrak {sl}}}_2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>U</mi> <mi>q</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mover accent="true"> <mi mathvariant="fraktur">sl</mi> <mo stretchy="true">^</mo> </mover> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, and the enveloping algebra of the Onsager Lie algebra. In this paper, we introduce the <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10801_2025_1420_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(S_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>S</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation>-symmetric tridiagonal algebra. This algebra has six generators. The generators can be identified with the vertices of a regular hexagon, such that nonadjacent generators commute and adjacent generators satisfy a pair of tridiagonal relations. For a <i>Q</i>-polynomial distance-regular graph <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10801_2025_1420_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation>, we turn the tensor power <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10801_2025_1420_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="TEX">\(V^{\otimes 3}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>V</mi> <mrow> <mo>⊗</mo> <mn>3</mn> </mrow> </msup> </math></EquationSource> </InlineEquation> of the standard module <i>V</i> into a module for an <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10801_2025_1420_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(S_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>S</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation>-symmetric tridiagonal algebra. We investigate in detail the case in which <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10801_2025_1420_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation> is a Hamming graph. We give some conjectures and open problems.</p>

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The \(S_3\)-symmetric tridiagonal algebra

  • Paul Terwilliger

摘要

The tridiagonal algebra is defined by two generators and two relations, called the tridiagonal relations. Special cases of the tridiagonal algebra include the q-Onsager algebra, the positive part of the q-deformed enveloping algebra \(U_q({\widehat{\mathfrak {sl}}}_2)\) U q ( sl ^ 2 ) , and the enveloping algebra of the Onsager Lie algebra. In this paper, we introduce the \(S_3\) S 3 -symmetric tridiagonal algebra. This algebra has six generators. The generators can be identified with the vertices of a regular hexagon, such that nonadjacent generators commute and adjacent generators satisfy a pair of tridiagonal relations. For a Q-polynomial distance-regular graph \(\Gamma \) Γ , we turn the tensor power \(V^{\otimes 3}\) V 3 of the standard module V into a module for an \(S_3\) S 3 -symmetric tridiagonal algebra. We investigate in detail the case in which \(\Gamma \) Γ is a Hamming graph. We give some conjectures and open problems.