{"title":"Conformal bootstrap equations from the embedding space operator product expansion","authors":"Jean-François Fortin, Wen-Jie Ma, Valentina Prilepina, Witold Skiba","doi":"10.1007/JHEP10(2024)245","DOIUrl":null,"url":null,"abstract":"<p>We describe how to implement the conformal bootstrap program in the context of the embedding space OPE formalism introduced in previous work. To take maximal advantage of the known properties of the scalar conformal blocks for symmetric-traceless exchange, we construct tensorial generalizations of the three-point and four-point scalar conformal blocks that have many nice properties. Further, we present a special basis of tensor structures for three-point correlation functions endowed with the remarkable simplifying property that it does not mix under permutations of the external quasi-primary operators. We find that in this approach, we can write the <i>M</i>-point conformal bootstrap equations explicitly in terms of the standard position space cross-ratios without the need to project back to position space, thus effectively deriving all conformal bootstrap equations directly from the embedding space. Finally, we lay out an algorithm for generating the conformal bootstrap equations in this formalism. Collectively, the tensorial generalizations, the new basis of tensor structures, as well as the procedure for deriving the conformal bootstrap equations lead to four-point bootstrap equations for quasi-primary operators in arbitrary Lorentz representations expressed as linear combinations of the standard scalar conformal blocks for spin-<i>ℓ</i> exchange, with finite <i>ℓ</i>-independent terms. Moreover, the OPE coefficients in these equations conveniently feature trivial symmetry properties. The only inputs necessary are the relevant projection operators and tensor structures, which are all fixed by group theory. To illustrate the procedure, we present one nontrivial example involving scalars <i>S</i> and vectors <i>V</i>, namely ⟨<i>SSSV</i>⟩.</p>","PeriodicalId":635,"journal":{"name":"Journal of High Energy Physics","volume":"2024 10","pages":""},"PeriodicalIF":5.4000,"publicationDate":"2024-10-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/JHEP10(2024)245.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of High Energy Physics","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/JHEP10(2024)245","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Physics and Astronomy","Score":null,"Total":0}
引用次数: 0
Abstract
We describe how to implement the conformal bootstrap program in the context of the embedding space OPE formalism introduced in previous work. To take maximal advantage of the known properties of the scalar conformal blocks for symmetric-traceless exchange, we construct tensorial generalizations of the three-point and four-point scalar conformal blocks that have many nice properties. Further, we present a special basis of tensor structures for three-point correlation functions endowed with the remarkable simplifying property that it does not mix under permutations of the external quasi-primary operators. We find that in this approach, we can write the M-point conformal bootstrap equations explicitly in terms of the standard position space cross-ratios without the need to project back to position space, thus effectively deriving all conformal bootstrap equations directly from the embedding space. Finally, we lay out an algorithm for generating the conformal bootstrap equations in this formalism. Collectively, the tensorial generalizations, the new basis of tensor structures, as well as the procedure for deriving the conformal bootstrap equations lead to four-point bootstrap equations for quasi-primary operators in arbitrary Lorentz representations expressed as linear combinations of the standard scalar conformal blocks for spin-ℓ exchange, with finite ℓ-independent terms. Moreover, the OPE coefficients in these equations conveniently feature trivial symmetry properties. The only inputs necessary are the relevant projection operators and tensor structures, which are all fixed by group theory. To illustrate the procedure, we present one nontrivial example involving scalars S and vectors V, namely ⟨SSSV⟩.
我们描述了如何在前人介绍的嵌入空间 OPE 形式的背景下实现共形引导程序。为了最大限度地利用对称无踪迹交换的标量共形块的已知特性,我们构建了三点和四点标量共形块的张量广义,它们具有许多很好的特性。此外,我们还为三点相关函数提出了一种特殊的张量结构基础,它具有显著的简化特性,即在外部准主算子的排列组合下不会混合。我们发现,在这种方法中,我们可以用标准位置空间交叉比明确地写出 M 点共形引导方程,而无需投影回位置空间,从而有效地直接从嵌入空间推导出所有共形引导方程。最后,我们提出了一种在此形式主义下生成共形引导方程的算法。总体而言,张量泛化、新的张量结构基础以及保角自举方程的推导过程,导致了任意洛伦兹表示中准主算子的四点自举方程,这些方程以自旋ℓ 交换的标准标量保角块的线性组合表示,并具有有限的ℓ 无关项。此外,这些方程中的 OPE 系数具有微不足道的对称性。唯一需要输入的是相关的投影算子和张量结构,这些都是由群论固定的。为了说明这个过程,我们举一个涉及标量 S 和矢量 V 的非微观例子,即⟨SSSV⟩。
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