<p>In this work, we investigate how the marginal beta deformation of the <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_26379_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">N</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{N} \)</EquationSource> </InlineEquation> = 4 super-Yang-Mills theory manifests within the context of the topological B-model in the twistor space <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_26379_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi mathvariant="double-struck">CP</mi> <mrow> <mfenced close="|"> <mn>3</mn> </mfenced> <mn>4</mn> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">\( {\mathbbm{CP}}^{\left.3\right|4} \)</EquationSource> </InlineEquation>. We begin by identifying the beta deformation as states living in a specific irreducible representation of the superconformal algebra. Then, we compute the ghost number two elements of the BRST cohomology of the topological model. A gauge-fixing procedure is applied to these states, allowing us to identify the elements living in the irreducible representation that characterizes the beta deformation. Based on this identification, we proceed to write the deformed topological action, and the corresponding deformed BRST operator.</p>

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Beta-deformation in twistor-string theory

  • Eggon Viana

摘要

In this work, we investigate how the marginal beta deformation of the N \( \mathcal{N} \) = 4 super-Yang-Mills theory manifests within the context of the topological B-model in the twistor space CP 3 4 \( {\mathbbm{CP}}^{\left.3\right|4} \) . We begin by identifying the beta deformation as states living in a specific irreducible representation of the superconformal algebra. Then, we compute the ghost number two elements of the BRST cohomology of the topological model. A gauge-fixing procedure is applied to these states, allowing us to identify the elements living in the irreducible representation that characterizes the beta deformation. Based on this identification, we proceed to write the deformed topological action, and the corresponding deformed BRST operator.