{"paper":{"title":"Semi-doubled Gauged Linear Sigma Model for Five-branes of Codimension Two","arxiv_id":"1810.02169","primary_cat":"hep-th","submitted_at":"2018-10-04T12:20:48+00:00","version_compiled":"v2"},"notice":"Every quoted sentence is the authors' text from the arXiv listing abstract. Labels and probabilities are the outputs of classifier-1.13.0 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 v2","sentences":[{"i":0,"p":0.96,"id":"s0","own":true,"role":"contribution","text":"We establish a double dualization in two-dimensional supersymmetric gauge theory.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.94,"main_claim_p":0.35,"quantitative":false,"quantitative_p":0.18,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.03,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.96,"interpretation":0.0}},{"i":1,"p":0.56,"id":"s1","own":true,"role":"method","text":"We construct a gauged linear sigma model (GLSM) which contains a complex twisted linear superfield coupled to two sets of Abelian vector superfields.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.95,"main_claim_p":0.06,"quantitative":false,"quantitative_p":0.49,"role_probabilities":{"gap":0.0,"method":0.56,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.44,"interpretation":0.0}},{"i":2,"p":0.92,"id":"s2","own":true,"role":"result","text":"In the IR regime, the GLSM provides a string sigma model whose target spaces are a defect NS5-brane, a Kaluza-Klein vortex and an exotic $5^2_2$-brane.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.9,"main_claim_p":0.37,"quantitative":false,"quantitative_p":0.22,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.92,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.08,"interpretation":0.0}},{"i":3,"p":0.75,"id":"s3","own":true,"role":"result","text":"All of them are five-branes of codimension two and are related by T-duality.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.61,"main_claim_p":0.19,"quantitative":true,"quantitative_p":0.59,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.75,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.01,"interpretation":0.24}},{"i":4,"p":0.84,"id":"s4","own":false,"role":"background","text":"This model is a natural extension of the GLSM proposed by Tong which gives a sigma model for an H-monopole, i.e., a smeared NS5-brane of codimension three.","hedge":{"p":0.99,"label":"asserted"},"own_p":0.19,"main_claim_p":0.06,"quantitative":true,"quantitative_p":0.55,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.0,"background":0.84,"limitation":0.0,"future_work":0.0,"contribution":0.09,"interpretation":0.06}},{"i":5,"p":0.41,"id":"s5","own":false,"role":"interpretation","text":"This is also regarded as an alternative system of the GLSM for exotic five-branes proposed by the present authors.","hedge":{"p":0.75,"label":"asserted"},"own_p":0.37,"main_claim_p":0.05,"quantitative":false,"quantitative_p":0.22,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.0,"background":0.4,"limitation":0.0,"future_work":0.0,"contribution":0.18,"interpretation":0.41}},{"i":6,"p":0.9,"id":"s6","own":true,"role":"result","text":"In this analysis, we confirm that the T-duality transformation procedure in terms of the complex twisted linear superfield is applicable to dualize both the real and imaginary parts of the twisted chiral superfield even at the UV level, beyond the IR limit.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.93,"main_claim_p":0.27,"quantitative":false,"quantitative_p":0.38,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.9,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.08,"interpretation":0.01}},{"i":7,"p":0.94,"id":"s7","own":true,"role":"interpretation","text":"This indicates that the T-duality transformations at finite gauge couplings can be performed in terms of reducible superfields in the same way as irreducible (twisted) chiral superfields.","hedge":{"p":0.91,"label":"hedged_possibility"},"own_p":0.79,"main_claim_p":0.2,"quantitative":false,"quantitative_p":0.44,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.06,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.94}},{"i":8,"p":0.97,"id":"s8","own":true,"role":"contribution","text":"Furthermore, we study quantum vortex corrections to the GLSM at the UV level.","hedge":{"p":0.92,"label":"asserted"},"own_p":0.94,"main_claim_p":0.05,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.03,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.97,"interpretation":0.0}},{"i":9,"p":0.87,"id":"s9","own":true,"role":"result","text":"In the IR limit, these corrections are mapped to string worldsheet instanton corrections to the five-branes of codimension 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