{"paper":{"title":"Adding new hair to the 3-charge black ring","arxiv_id":"1201.2585","primary_cat":"hep-th","submitted_at":"2012-01-12T15:08:37+00:00","version_compiled":"v1"},"notice":"Every quoted sentence is the authors' text from the arXiv listing abstract. Labels and probabilities are the outputs of classifier-1.13-20260917 on the question bank abstract-p1-20260923, exactly as returned. No sentence in this record was written by a language model.","schema":"pith.compiled-record/v0","status":"compiled","abstract":{"source":"arXiv listing abstract v1","sentences":[{"i":0,"p":0.98,"id":"s0","own":true,"role":"contribution","text":"Motivated by the string theory analysis of arXiv:1108.6331, we construct a class of 1/8-BPS solutions of type IIB supergravity compactified on S^1 x T^4.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.94,"main_claim_p":0.08,"quantitative":true,"quantitative_p":0.82,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.0,"background":0.02,"limitation":0.0,"future_work":0.0,"contribution":0.98,"interpretation":0.0}},{"i":1,"p":0.53,"id":"s1","own":false,"role":"contribution","text":"In this duality frame our ansatz allows for a non-trivial NS-NS B-field which has been usually set to zero in previous studies of 1/8-BPS geometries.","hedge":{"p":0.99,"label":"asserted"},"own_p":0.47,"main_claim_p":0.07,"quantitative":false,"quantitative_p":0.32,"role_probabilities":{"gap":0.31,"method":0.15,"result":0.0,"background":0.01,"limitation":0.0,"future_work":0.0,"contribution":0.53,"interpretation":0.0}},{"i":2,"p":0.47,"id":"s2","own":true,"role":"interpretation","text":"We provide a M-theory description of these new geometries and show that they can be interpreted as the lift of solutions of the N=2 5D supergravity with three vector multiplets and whose scalar manifold is the symmetric space SO(1,1) x (SO(1,2)/SO(2)).","hedge":{"p":1.0,"label":"asserted"},"own_p":0.93,"main_claim_p":0.17,"quantitative":false,"quantitative_p":0.48,"role_probabilities":{"gap":0.0,"method":0.02,"result":0.08,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.43,"interpretation":0.47}},{"i":3,"p":0.68,"id":"s3","own":true,"role":"result","text":"Finally we show that the non-minimal 5D black rings provide an explicit example of solutions falling in this ansatz.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.94,"main_claim_p":0.25,"quantitative":false,"quantitative_p":0.24,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.68,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.29,"interpretation":0.03}},{"i":4,"p":0.91,"id":"s4","own":true,"role":"result","text":"In particular we point out the existence of a black ring that has an extra dipole charge with respect to the solutions of the STU-model.","hedge":{"p":0.97,"label":"asserted"},"own_p":0.91,"main_claim_p":0.3,"quantitative":true,"quantitative_p":0.7,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.91,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.09,"interpretation":0.0}},{"i":5,"p":0.88,"id":"s5","own":true,"role":"interpretation","text":"In the near-horizon limit, this ring has an AdS_3 x S^3 geometry with the same radius as the one of the 3-charge black hole and thus its microstates should belong to the usual D1-D5 CFT.","hedge":{"p":0.45,"label":"asserted"},"own_p":0.88,"main_claim_p":0.21,"quantitative":true,"quantitative_p":0.94,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.12,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.88}}]},"compiled":{"main_claim":{"p":0.55,"text":"In particular we point out the existence of a black ring that has an extra dipole charge with respect to the solutions of the STU-model.","location":"abstract s4","hedge_strength":{"p":0.97,"label":"asserted"}},"provenance":{"route":{"via":"OpenRouter","model":"classifier-1.13","endpoint":"https://openrouter.ai/api/v1/systemone","provider":"TypeSafe"},"packing":"one request per 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