<p>We construct the <i>q</i>-deformed Clifford algebra of&#xa0;<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathfrak {sl}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> and study its properties. This allows us to define the <i>q</i>-deformed noncommutative Weil algebra&#xa0;<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq5.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {W}_q(\mathfrak {sl}_2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">W</mi> <mi>q</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for&#xa0;<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq6.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\(U_q(\mathfrak {sl}_2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>U</mi> <mi>q</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and the corresponding cubic Dirac operator&#xa0;<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(D_q\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>D</mi> <mi>q</mi> </msub> </math></EquationSource> </InlineEquation>. In the classical case this was done by Alekseev and Meinrenken in&#xa0;2000. We show that the cubic Dirac operator&#xa0;<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(D_q\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>D</mi> <mi>q</mi> </msub> </math></EquationSource> </InlineEquation> is invariant with respect to the <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq9.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\(U_q({\mathfrak {sl}}_2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>U</mi> <mi>q</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>-action and <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq10.gif" Format="GIF" Height="9" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow /> <mo>∗</mo> </mrow> </math></EquationSource> </InlineEquation>-structures on&#xa0;<InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq11.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {W}_q(\mathfrak {sl}_2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">W</mi> <mi>q</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, moreover, the square of&#xa0;<InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq12.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(D_q\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>D</mi> <mi>q</mi> </msub> </math></EquationSource> </InlineEquation> is central in&#xa0;<InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq13.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {W}_q(\mathfrak {sl}_2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">W</mi> <mi>q</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. We compute the spectrum of the cubic element on finite-dimensional and Verma modules of&#xa0;<InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="6_2025_1372_Article_IEq14.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\(U_q(\mathfrak {sl}_2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>U</mi> <mi>q</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and the corresponding Dirac cohomology.</p>

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Cubic Dirac operator for \(U_q({\mathfrak {sl}}_2)\)

  • Andrey Krutov,
  • Pavle Pandžić

摘要

We construct the q-deformed Clifford algebra of  \(\mathfrak {sl}_2\) sl 2 and study its properties. This allows us to define the q-deformed noncommutative Weil algebra  \(\mathcal {W}_q(\mathfrak {sl}_2)\) W q ( sl 2 ) for  \(U_q(\mathfrak {sl}_2)\) U q ( sl 2 ) and the corresponding cubic Dirac operator  \(D_q\) D q . In the classical case this was done by Alekseev and Meinrenken in 2000. We show that the cubic Dirac operator  \(D_q\) D q is invariant with respect to the \(U_q({\mathfrak {sl}}_2)\) U q ( sl 2 ) -action and \(*\) -structures on  \(\mathcal {W}_q(\mathfrak {sl}_2)\) W q ( sl 2 ) , moreover, the square of  \(D_q\) D q is central in  \(\mathcal {W}_q(\mathfrak {sl}_2)\) W q ( sl 2 ) . We compute the spectrum of the cubic element on finite-dimensional and Verma modules of  \(U_q(\mathfrak {sl}_2)\) U q ( sl 2 ) and the corresponding Dirac cohomology.