<p>It is known that the <i>q</i>-deformed Virasoro algebra can be constructed from a certain representation of the quantum toroidal <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq3.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathfrak {gl}_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">gl</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> algebra. In this paper, we apply the same construction to the quantum toroidal algebra of type <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq1.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathfrak {gl}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">gl</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> and study the properties of resulting generators <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(W_i(z)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>W</mi> <mi>i</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> (<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq6.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="TEX">\(i=1,2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>). The algebra generated by <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(W_i(z)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>W</mi> <mi>i</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> can be regarded as a <i>q</i>-deformation of the direct sum <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq8.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textsf{F} \oplus \textsf{SVir}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="sans-serif">F</mi> <mo>⊕</mo> <mi mathvariant="sans-serif">SVir</mi> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq9.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textsf{F}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="sans-serif">F</mi> </math></EquationSource> </InlineEquation> denotes the free fermion algebra and <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textsf{SVir}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="sans-serif">SVir</mi> </math></EquationSource> </InlineEquation> stands for the <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq11.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(N=1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> super Virasoro algebra, also referred to as the <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq11.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(N=1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> superconformal algebra or the Neveu–Schwarz–Ramond algebra. Moreover, the generators <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(W_i(z)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>W</mi> <mi>i</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> admit two screening currents, and we show that their degeneration limits coincide with the screening currents of <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textsf{SVir}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="sans-serif">SVir</mi> </math></EquationSource> </InlineEquation>. We also establish quadratic relations satisfied by <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(W_i(z)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>W</mi> <mi>i</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and show that they generate a pair of commuting <i>q</i>-deformed Virasoro algebras, which degenerate into two nontrivial commuting Virasoro algebras included in <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1997_Article_IEq8.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\textsf{F} \oplus \textsf{SVir}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="sans-serif">F</mi> <mo>⊕</mo> <mi mathvariant="sans-serif">SVir</mi> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Direct sum structure of the super Virasoro algebra and a Fermion algebra arising from the quantum toroidal \(\mathfrak {gl}_2\)

  • Yusuke Ohkubo

摘要

It is known that the q-deformed Virasoro algebra can be constructed from a certain representation of the quantum toroidal \(\mathfrak {gl}_1\) gl 1 algebra. In this paper, we apply the same construction to the quantum toroidal algebra of type \(\mathfrak {gl}_2\) gl 2 and study the properties of resulting generators \(W_i(z)\) W i ( z ) ( \(i=1,2\) i = 1 , 2 ). The algebra generated by \(W_i(z)\) W i ( z ) can be regarded as a q-deformation of the direct sum \(\textsf{F} \oplus \textsf{SVir}\) F SVir , where \(\textsf{F}\) F denotes the free fermion algebra and \(\textsf{SVir}\) SVir stands for the \(N=1\) N = 1 super Virasoro algebra, also referred to as the \(N=1\) N = 1 superconformal algebra or the Neveu–Schwarz–Ramond algebra. Moreover, the generators \(W_i(z)\) W i ( z ) admit two screening currents, and we show that their degeneration limits coincide with the screening currents of \(\textsf{SVir}\) SVir . We also establish quadratic relations satisfied by \(W_i(z)\) W i ( z ) and show that they generate a pair of commuting q-deformed Virasoro algebras, which degenerate into two nontrivial commuting Virasoro algebras included in \(\textsf{F} \oplus \textsf{SVir}\) F SVir .