<p>We construct highest weight vectors of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5252_Article_IEq3.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="87" /> </InlineMediaObject> <EquationSource Format="TEX">\(\widehat{\mathfrak {sl}_2}_{,k+1} \oplus \textsf{Vir}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mover accent="true"> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="true">^</mo> </mover> <mrow> <mo>,</mo> <mi>k</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>⊕</mo> <mi mathvariant="sans-serif">Vir</mi> </mrow> </math></EquationSource> </InlineEquation> in tensor products of highest weight modules of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5252_Article_IEq4.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\(\widehat{\mathfrak {sl}_2}_{,k}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover accent="true"> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="true">^</mo> </mover> <mrow> <mo>,</mo> <mi>k</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5252_Article_IEq5.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="TEX">\(\widehat{\mathfrak {sl}_2}_{,1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover accent="true"> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="true">^</mo> </mover> <mrow> <mo>,</mo> <mn>1</mn> </mrow> </msub> </math></EquationSource> </InlineEquation>, and thus for generic weights we find the decomposition of the tensor product into irreducibles of <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5252_Article_IEq6.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="84" /> </InlineMediaObject> <EquationSource Format="TEX">\(\widehat{\mathfrak {sl}_2}_{k+1} \oplus \textsf{Vir}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mover accent="true"> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="true">^</mo> </mover> <mrow> <mi>k</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>⊕</mo> <mi mathvariant="sans-serif">Vir</mi> </mrow> </math></EquationSource> </InlineEquation>. The construction uses Wakimoto representations of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="220_2025_5252_Article_IEq7.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\(\widehat{\mathfrak {sl}_2}_{,k}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover accent="true"> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mo stretchy="true">^</mo> </mover> <mrow> <mo>,</mo> <mi>k</mi> </mrow> </msub> </math></EquationSource> </InlineEquation>, but the obtained vectors can be mapped back to Verma modules. Singularities of this mapping are cancelled by a renormalization. A detailed study of “degenerations” of Wakimoto modules allowed to find the renormalization factor explicitly. The obtained result is a&#xa0;significant step forward in a proof of equivalence of certain two-dimensional CFT models.</p>

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Decomposition of \(\widehat{\mathfrak {sl}_2} _{,k} \ \oplus \ \widehat{\mathfrak {sl}_2} _{,1}\) Highest Weight Representations for Generic Level k and Equivalence Between Two-Dimensional CFT Models

  • Leszek Hadasz,
  • Błażej Ruba

摘要

We construct highest weight vectors of \(\widehat{\mathfrak {sl}_2}_{,k+1} \oplus \textsf{Vir}\) sl 2 ^ , k + 1 Vir in tensor products of highest weight modules of \(\widehat{\mathfrak {sl}_2}_{,k}\) sl 2 ^ , k and \(\widehat{\mathfrak {sl}_2}_{,1}\) sl 2 ^ , 1 , and thus for generic weights we find the decomposition of the tensor product into irreducibles of \(\widehat{\mathfrak {sl}_2}_{k+1} \oplus \textsf{Vir}\) sl 2 ^ k + 1 Vir . The construction uses Wakimoto representations of \(\widehat{\mathfrak {sl}_2}_{,k}\) sl 2 ^ , k , but the obtained vectors can be mapped back to Verma modules. Singularities of this mapping are cancelled by a renormalization. A detailed study of “degenerations” of Wakimoto modules allowed to find the renormalization factor explicitly. The obtained result is a significant step forward in a proof of equivalence of certain two-dimensional CFT models.