<p>In recent work, Lusztig’s positive root vectors (with respect to a distinguished choice of reduced decomposition of the longest element of the Weyl group) were shown to give a quantum tangent space for every <i>A</i>-series Drinfeld–Jimbo full quantum flag manifold <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1955_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {O}_q(\textrm{F}_n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">O</mi> <mi>q</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mtext>F</mtext> <mi>n</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. Moreover, the associated differential calculus <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1955_Article_IEq5.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="68" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega ^{(0,\bullet )}_q(\textrm{F}_n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi mathvariant="normal">Ω</mi> <mi>q</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mo>∙</mo> <mo stretchy="false">)</mo> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <msub> <mtext>F</mtext> <mi>n</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> was shown to have classical dimension, giving a direct <i>q</i>-deformation of the classical anti-holomorphic Dolbeault complex of <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1955_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textrm{F}_n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>F</mtext> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation>. Here, we examine in detail the rank two case, namely the full quantum flag manifold of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1955_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {O}_q(\textrm{SU}_3)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">O</mi> <mi>q</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mtext>SU</mtext> <mn>3</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. In particular, we examine the <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1955_Article_IEq8.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>-differential calculus associated with <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1955_Article_IEq9.gif" Format="GIF" Height="24" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega ^{(0,\bullet )}_q(\textrm{F}_3)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi mathvariant="normal">Ω</mi> <mi>q</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mo>∙</mo> <mo stretchy="false">)</mo> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <msub> <mtext>F</mtext> <mn>3</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and its noncommutative complex geometry. We find that the number of almost-complex structures reduces from 8 (that is 2 to the power of the number of positive roots of <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1955_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathfrak {sl}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">sl</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation>) to 4 (that is 2 to the power of the number of simple roots of <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1955_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathfrak {sl}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">sl</mi> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation>). Moreover, we show that each of these almost-complex structures is integrable, which is to say, each of them is a complex structure. Finally, we observe that, due to non-centrality of all the non-degenerate coinvariant 2-forms, none of these complex structures admits a left <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1955_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {O}_q(\textrm{SU}_3)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">O</mi> <mi>q</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msub> <mtext>SU</mtext> <mn>3</mn> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>-covariant noncommutative Kähler structure.</p>

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Noncommutative complex structures for the full quantum flag manifold of \(\mathcal {O}_q(\textrm{SU}_3)\)

  • Alessandro Carotenuto,
  • Réamonn Ó Buachalla,
  • Junaid Razzaq

摘要

In recent work, Lusztig’s positive root vectors (with respect to a distinguished choice of reduced decomposition of the longest element of the Weyl group) were shown to give a quantum tangent space for every A-series Drinfeld–Jimbo full quantum flag manifold \(\mathcal {O}_q(\textrm{F}_n)\) O q ( F n ) . Moreover, the associated differential calculus \(\Omega ^{(0,\bullet )}_q(\textrm{F}_n)\) Ω q ( 0 , ) ( F n ) was shown to have classical dimension, giving a direct q-deformation of the classical anti-holomorphic Dolbeault complex of \(\textrm{F}_n\) F n . Here, we examine in detail the rank two case, namely the full quantum flag manifold of \(\mathcal {O}_q(\textrm{SU}_3)\) O q ( SU 3 ) . In particular, we examine the \(*\) -differential calculus associated with \(\Omega ^{(0,\bullet )}_q(\textrm{F}_3)\) Ω q ( 0 , ) ( F 3 ) and its noncommutative complex geometry. We find that the number of almost-complex structures reduces from 8 (that is 2 to the power of the number of positive roots of \(\mathfrak {sl}_3\) sl 3 ) to 4 (that is 2 to the power of the number of simple roots of \(\mathfrak {sl}_3\) sl 3 ). Moreover, we show that each of these almost-complex structures is integrable, which is to say, each of them is a complex structure. Finally, we observe that, due to non-centrality of all the non-degenerate coinvariant 2-forms, none of these complex structures admits a left \(\mathcal {O}_q(\textrm{SU}_3)\) O q ( SU 3 ) -covariant noncommutative Kähler structure.