{"title":"Leading large N giant graviton correction to Schur correlators in large representations","authors":"","doi":"10.1016/j.nuclphysb.2024.116638","DOIUrl":null,"url":null,"abstract":"<div><p>We consider 4d <span><math><mi>N</mi><mo>=</mo><mn>4</mn></math></span> <span><math><mi>U</mi><mo>(</mo><mi>N</mi><mo>)</mo></math></span> SYM and the leading giant graviton correction at large <em>N</em> to the Schur defect 2-point functions of <span><math><mfrac><mrow><mn>1</mn></mrow><mrow><mn>2</mn></mrow></mfrac></math></span>-BPS Wilson lines in rank-<em>k</em> symmetric and antisymmetric representations. We study in particular the large <em>k</em> limit for the symmetric case and the regime <span><math><mn>1</mn><mo>≪</mo><mi>k</mi><mo>≪</mo><mi>N</mi></math></span> in the antisymmetric one. In both cases we present exact results for the correction. Wilson lines in symmetric/antisymmetric representations admit a description in terms of D3<sub><em>k</em></sub> and D5<sub><em>k</em></sub> brane probes representing a collection of <em>k</em> fundamental strings. In this picture, giant graviton corrections come from fluctuations of brane probes in the presence of a wrapped D3 brane giant graviton. In the antisymmetric case, our leading correction matches the half-index of the 4d <span><math><mi>N</mi><mo>=</mo><mn>4</mn></math></span> Maxwell theory living on the disk which is a part of the giant graviton divided out by the D5<sub><em>k</em></sub> probe, as recently proposed in <span><span>arXiv:2404.08302</span><svg><path></path></svg></span>. For the symmetric case at large <em>k</em>, we derive an explicit exact residue formula for the leading large <em>N</em> correction.</p></div>","PeriodicalId":54712,"journal":{"name":"Nuclear Physics B","volume":null,"pages":null},"PeriodicalIF":2.5000,"publicationDate":"2024-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0550321324002049/pdfft?md5=9e35a9f3b5e8b21a8c9a497f408e0648&pid=1-s2.0-S0550321324002049-main.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Physics B","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0550321324002049","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
引用次数: 0
Abstract
We consider 4d SYM and the leading giant graviton correction at large N to the Schur defect 2-point functions of -BPS Wilson lines in rank-k symmetric and antisymmetric representations. We study in particular the large k limit for the symmetric case and the regime in the antisymmetric one. In both cases we present exact results for the correction. Wilson lines in symmetric/antisymmetric representations admit a description in terms of D3k and D5k brane probes representing a collection of k fundamental strings. In this picture, giant graviton corrections come from fluctuations of brane probes in the presence of a wrapped D3 brane giant graviton. In the antisymmetric case, our leading correction matches the half-index of the 4d Maxwell theory living on the disk which is a part of the giant graviton divided out by the D5k probe, as recently proposed in arXiv:2404.08302. For the symmetric case at large k, we derive an explicit exact residue formula for the leading large N correction.
期刊介绍:
Nuclear Physics B focuses on the domain of high energy physics, quantum field theory, statistical systems, and mathematical physics, and includes four main sections: high energy physics - phenomenology, high energy physics - theory, high energy physics - experiment, and quantum field theory, statistical systems, and mathematical physics. The emphasis is on original research papers (Frontiers Articles or Full Length Articles), but Review Articles are also welcome.