Scholarlink

<p>We construct AdS<sub>5</sub> × Σ solutions of <i>D</i> = 7 gauged supergravity where Σ is a disc, also known as a half-spindle, and uplift them to <i>D</i> = 11 supergravity. By computing the anomaly polynomial of the M5-brane theory compactified on Σ in the large <i>N</i> limit, we obtain the off-shell central charges of the dual <i>D</i> = 4, <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27378_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> = 1 superconformal field theory to disc solutions. These off-shell central charges decompose into contributions from the center and the boundary of the disc and are referred to as the gravitational blocks for disc. By suitably gluing the gravitational blocks for two discs along their boundaries, we reproduce the off-shell central charge for a single spindle.</p>

错误：搜索内容不能为空，请输入英文关键词
错误：关键词超出字数限制，请精简
高级检索

Gluing two discs into a spindle

  • 期刊论文

  • 出版模式：

    开放获取

  • 发表日期：

    2025年10月10日

查看全文
  • Hyojoong Kim,
  • Nakwoo Kim

摘要

We construct AdS5 × Σ solutions of D = 7 gauged supergravity where Σ is a disc, also known as a half-spindle, and uplift them to D = 11 supergravity. By computing the anomaly polynomial of the M5-brane theory compactified on Σ in the large N limit, we obtain the off-shell central charges of the dual D = 4, N \( \mathcal{N} \) = 1 superconformal field theory to disc solutions. These off-shell central charges decompose into contributions from the center and the boundary of the disc and are referred to as the gravitational blocks for disc. By suitably gluing the gravitational blocks for two discs along their boundaries, we reproduce the off-shell central charge for a single spindle.