{"arxiv_id":"hep-th/0603013","incoming":{"papers":82,"sentences":138,"groups":[{"kind":"extends","label":"Builds on it","papers":4,"sentences":4,"quotes":[{"arxiv_id":"0804.2907","title":"Janus Configurations, Chern-Simons Couplings, And The Theta-Angle in N=4 Super Yang-Mills Theory","url":"/paper/0804.2907","section":"Conformally Invariant Limit","sentence":"Now (generalizing section 6 of [ref] ) we would like to ask whether, classically, it is possible to take a limit in which the Janus configuration becomes conformally invariant.","intent_p":0.94,"contests_p":null},{"arxiv_id":"1107.2796","title":"Supersymmetric Janus solutions in five and ten dimensions","url":"/paper/1107.2796","section":"Introduction","sentence":"Later, the Janus field theories in [ref] were generalized to allow the theta-angle to vary which is holographicallly dual to the axion field, and were also applied to construct three-dimensional Chern-Simons theories with $𝒩$ = 4 supersymmetries in [ref] .","intent_p":0.82,"contests_p":null},{"arxiv_id":"0705.0024","title":"Exact half-BPS Type IIB interface solutions II: Flux solutions and multi-Janus","url":"/paper/0705.0024","section":"Introduction","sentence":"In section 8, a dual gauge theory is proposed as a generalization of the interface conformal field theory discussed in [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"2103.10797","title":"Global Properties of the Conformal Manifold for S-Fold Backgrounds","url":"/paper/2103.10797","section":"Introduction","sentence":"Furthermore, by translating this procedure on the corresponding $𝒩=4$ CFT$_3$ Janus-type theories [ref] [ref] , they were able to find strong candidates for their SCFT$_3$ duals.","intent_p":0.84,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":2,"quotes":[{"arxiv_id":"0807.3720","title":"S-Duality of Boundary Conditions In N=4 Super Yang-Mills Theory","url":"/paper/0807.3720","section":"Introduction","sentence":"The key step is to generalize $T(SU(n))$ and its close cousins, which we do using Janus domain walls [ref] .","intent_p":0.84,"contests_p":null},{"arxiv_id":"0904.3313","title":"Janus solutions in M-theory","url":"/paper/0904.3313","section":"Discussion","sentence":"For example, application of the methods developed in [ref] could be used to calculate correlation functions in the presence of the interface/defect. * As the ABJM theory enjoys a well-understood field theoretic CFT description, one may classify the possible interface/defect terms along the lines of [ref] and [ref] , establish their symmetries, and derive the associated supergravity solutions. * In Type IIB theory, the simplest Janus solution breaks all supersymmetries, has a non-trivial dilaton profile, and vanishing 3-form flux fields.","intent_p":0.81,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":5,"sentences":5,"quotes":[{"arxiv_id":"0802.2143","title":"Janus and Multifaced Supersymmetric Theories","url":"/paper/0802.2143","section":"Additional Susy Breaking Janus","sentence":"We easily recover the results in Ref. [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"1609.05905","title":"Supergravity Backgrounds for Four-Dimensional Maximally Supersymmetric Yang-Mills","url":"/paper/1609.05905","section":"Janus examples","sentence":"To compare with [ref] , we will look for solutions to eq:susyconditions satisfying the following input assumptions: first, the solutions exist in Minkowski spacetime with the trivial metric, and they preserve a three-dimensional Poincare symmetry.","intent_p":0.96,"contests_p":null},{"arxiv_id":"2204.09993","title":"Type IIB S-folds: flat deformations, holography and stability","url":"/paper/2204.09993","section":"Flat deformations of type IIB S-folds: four-dimensional picture","sentence":"The symmetries of these solutions nicely match with the largest symmetric SYM interfaces classified in [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"2007.15095","title":"Spatially modulated and supersymmetric mass deformations of $\\mathcal{N}=4$ SYM","url":"/paper/2007.15095","section":"Introduction","sentence":"At this point it is worth emphasising that our field theory results concerning supersymmetric Janus configurations of $𝒩=4$ SYM with constant coupling across the interface are complementary to the classification carried out in [ref] , for which it was assumed that the coupling constant varies across the interface and that any additional deformations are proportional to the spatial derivative of the coupling constant.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1610.07983","title":"Supersymmetric deformations of 3D SCFTs from tri-sasakian truncation","url":"/paper/1610.07983","section":"Conclusions","sentence":"This is similar to the five-dimensional Janus solution with unbroken $SO(6)$ symmetry [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2003.09154","title":"Holographic Interfaces in N=4 SYM: Janus and J-folds","url":"/paper/2003.09154","section":"The five-dimensional Janus","sentence":"Furthermore, from the presence of nontrivial bosonic and fermionic bilinear operators in the dual field theory [ref] , we deduce that the corresponding scalars, $α$ and $χ$, should both have non-trivial profiles and vanish in the AdS$_5$ asymptotic regions.","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":44,"sentences":44,"quotes":[{"arxiv_id":"1107.2796","title":"Supersymmetric Janus solutions in five and ten dimensions","url":"/paper/1107.2796","section":"Introduction","sentence":"Later, Janus gauge theories were constructed more systematically in [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"1804.06419","title":"Holographic duals of 3d S-fold CFTs","url":"/paper/1804.06419","section":"Supergravity solutions","sentence":"It was introduced in [ref] and generalized in [ref] .[See also [ref] for other studies of the supersymmetric Janus theory.] The holographic dual background corresponds to a solution with $Σ$ an infinite strip, which is shown in Figure [ref].","intent_p":0.88,"contests_p":null},{"arxiv_id":"2207.14015","title":"S-folds and $AdS_{3}$ flows from the D3-brane","url":"/paper/2207.14015","section":"Introduction","sentence":"Via the AdS/CFT correspondence [ref] , Janus solutions of supergravity theories [ref] provide a simple and explicit realisation of interfaces in dual field theories [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"1109.1927","title":"Holographic Interface-Particle Potential","url":"/paper/1109.1927","section":"Introduction and summary","sentence":"The supergravity description, sometimes called “Janus,” has been successfully constructed [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"2407.21619","title":"Half-BPS Janus solutions in AdS$_7$","url":"/paper/2407.21619","section":"Introduction","sentence":"The prototypical realisation of this is the Janus solution [ref] describing a one-parameter deformation of the $AdS_5×S^5$ vacuum of type IIB supergravity.","intent_p":0.82,"contests_p":null}]}],"unlabelled_sentences":82},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":{"arxiv_id":"hep-th/0603013","kind":"model","paper_version":1,"prompt_version":"held-up-v3.5","generated_at":"2026-10-27T18:51:15+00:00","loaded_at":"2026-10-28T01:03:17.987406+00:00","evidence":"substantial","account":[],"groups":[{"kind":"extends","label":"Builds on it","papers":2,"entries":[{"p":0.94,"quote":null,"citing":[{"self":false,"year":2008,"title":"Janus Configurations, Chern-Simons Couplings, And The Theta-Angle in N=4 Super Yang-Mills Theory","arxiv_id":"0804.2907"}],"verified":true,"paraphrase":"Generalized section 6 of this paper to ask whether the Janus configuration can classically be taken to a conformally invariant limit."}],"papers_all":4,"self_papers":1,"self_entries":[{"p":0.94,"quote":null,"citing":[{"self":true,"year":2007,"title":"Exact half-BPS Type IIB interface solutions II: Flux solutions and multi-Janus","arxiv_id":"0705.0024"}],"verified":true,"paraphrase":"Proposed a dual gauge theory as a generalization of the interface conformal field theory discussed in this paper."}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"entries":[{"p":0.99,"quote":null,"citing":[{"self":false,"year":2020,"title":"Holographic Interfaces in N=4 SYM: Janus and J-folds","arxiv_id":"2003.09154"}],"verified":true,"paraphrase":"Deduced from the nontrivial bosonic and fermionic bilinear operators in the dual field theory given in this paper that the scalars should have non-trivial profiles and vanish in the AdS5 asymptotic regions."}],"papers_all":1,"self_papers":0,"self_entries":[]}],"counts":{"by_kind":{"extends":4,"comparison":5,"method_or_tool":2,"supports_this_paper":1},"dropped":{"relied_on":0,"unknown_ids":0,"account_lines":0,"contest_vetoed":0,"below_threshold":0,"contest_drawback":0,"contest_without_basis":0,"contest_not_one_sentence":0,"contest_on_group_citation":0},"papers_read":16,"self_papers":16,"citing_papers":82,"sentences_read":30,"citing_sentences":140,"unambiguous_read":30,"typed_independent":10,"independent_papers":66,"by_kind_independent":{"extends":3,"comparison":5,"method_or_tool":1,"supports_this_paper":1}},"input_sha256":"3a955ffccf02bd0e44e6f3796e646d829afbe4d82e104d756dfcda043e3ac04e","method":"For a paper with five or more citing arXiv papers, Pith selected up to 40 citing sentences its citation classifier typed, read those whose citation markers point at this paper alone, and wrote one paraphrase for each later paper in each group, each resting on one sentence. A later paper is listed under a label only when the classifier gives one of its sentences that label at intent probability 0.8 or more (0.95 for support), Pith's reading of the sentence finds that the citing paper itself did it, and a second check of the paraphrase against the sentence passes. The section lists uses only: building on the paper, using its method, tool, data or values, comparing with it and citing it as support. It does not list criticism or disagreement, so their absence says nothing about how the paper has been received. Code counted the papers, wrote the summary from the listed entries, set the evidence level and linked each entry to its citing paper. Quotes are copied from the citing sentence and shown only when the citing paper's licence is CC BY, CC BY-SA or CC0; otherwise the paraphrase is shown. Papers that share an author with this one are listed apart. A paper with fewer citing papers gets a line counted by code, which names uses only: a later paper whose only label is a contest is counted as not described.","line":null,"summary":"2 later papers by other authors are listed below: 1 built on it and 1 cited it as support. 1 more paper by the same authors is listed: 1 built on it."},"_links":{"html":"https://pith.science/paper/hep-th/0603013"}}