{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1363670321170198656.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1007/jhep12(2016)103"}},{"identifier":{"@type":"URI","@value":"http://link.springer.com/content/pdf/10.1007/JHEP12(2016)103.pdf"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1610.05311"}}],"dc:title":[{"@value":"N $$ \\mathcal{N} $$ =1 Deformations and RG flows of N $$ \\mathcal{N} $$ =2 SCFTs, part II: non-principal deformations"}],"description":[{"notation":[{"@value":"We continue to investigate the $\\mathcal{N}=1$ deformations of four-dimensional $\\mathcal{N}=2$ superconformal field theories (SCFTs) labeled by a nilpotent element of the flavor symmetry. This triggers a renormalization group (RG) flow to an $\\mathcal{N}=1$ SCFT. We systematically analyze all possible deformations of this type for certain classes of $\\mathcal{N}=2$ SCFTs: conformal SQCDs, generalized Argyres-Douglas theories and the $E_6$ SCFT. We find a number of examples where the amount of supersymmetry gets enhanced to $\\mathcal{N}=2$ at the end point of the RG flow. Most notably, we find that the $SU(N)$ and $Sp(N)$ conformal SQCDs can be deformed to flow to the Argyres-Douglas (AD) theories of type $(A_1, D_{2N-1})$ and $(A_1, D_{2N})$ respectively. This RG flow therefore allows us to compute the full superconformal index of the $(A_1,D_N)$ class of AD theories. Moreover, we find an infrared duality between $\\mathcal{N}=1$ theories where the fixed point is described by an $\\mathcal{N}=2$ AD theory. We observe that the classes of examples that exhibit supersymmetry enhancement saturate certain bounds for the central charges implied by the associated two-dimensional chiral algebra."}]},{"notation":[{"@value":"46 pages, 12 tables, typos corrected and some minor changes"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1383670321170198656","@type":"Researcher","foaf:name":[{"@value":"Prarit Agarwal"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670321170198657","@type":"Researcher","foaf:name":[{"@value":"Kazunobu Maruyoshi"}]},{"@id":"https://cir.nii.ac.jp/crid/1383670321170198658","@type":"Researcher","foaf:name":[{"@value":"Jaewon Song"}]}],"publication":{"publicationIdentifier":[{"@type":"EISSN","@value":"10298479"}],"prism:publicationName":[{"@value":"Journal of High Energy Physics"}],"dc:publisher":[{"@value":"Springer Science and Business Media LLC"}],"prism:publicationDate":"2016-12","prism:volume":"2016","prism:number":"12","prism:startingPage":"103"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","url":[{"@id":"http://link.springer.com/content/pdf/10.1007/JHEP12(2016)103.pdf"}],"createdAt":"2016-12-22","modifiedAt":"2019-09-16","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Theory","dc:title":"High Energy Physics - Theory"},{"@id":"https://cir.nii.ac.jp/all?q=Nuclear%20and%20High%20Energy%20Physics","dc:title":"Nuclear and High Energy Physics"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Theory%20(hep-th)","dc:title":"High Energy Physics - Theory (hep-th)"},{"@id":"https://cir.nii.ac.jp/all?q=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360004235049585280","@type":"Article","resourceType":"学術雑誌論文(journal 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