{"paper":{"title":"Branes in Supergroups","arxiv_id":"0908.1816","primary_cat":"hep-th","submitted_at":"2009-08-13T16:22:12+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":0.99,"id":"s0","own":true,"role":"contribution","text":"In this thesis we initiate a systematic study of branes in Wess-Zumino-Novikov-Witten models with Lie supergroup target space.","hedge":{"p":0.96,"label":"asserted"},"own_p":0.89,"main_claim_p":0.06,"quantitative":false,"quantitative_p":0.03,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.0,"background":0.01,"limitation":0.0,"future_work":0.0,"contribution":0.99,"interpretation":0.0}},{"i":1,"p":0.55,"id":"s1","own":true,"role":"contribution","text":"We start by showing that a branes' worldvolume is a twisted superconjugacy class and construct the action of the boundary WZNW model.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.95,"main_claim_p":0.13,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.44,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.55,"interpretation":0.0}},{"i":2,"p":0.86,"id":"s2","own":true,"role":"contribution","text":"Then we consider symplectic fermions and give a complete description of boundary states including twisted sectors.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.93,"main_claim_p":0.08,"quantitative":false,"quantitative_p":0.07,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.13,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.86,"interpretation":0.0}},{"i":3,"p":0.89,"id":"s3","own":true,"role":"result","text":"Further we show that the GL(1|1) WZNW model is equivalent to symplectic fermions plus two scalars.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.87,"main_claim_p":0.11,"quantitative":false,"quantitative_p":0.37,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.89,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.11,"interpretation":0.0}},{"i":4,"p":0.9,"id":"s4","own":true,"role":"contribution","text":"We then consider the GL(1|1) boundary theory.","hedge":{"p":0.52,"label":"unclear"},"own_p":0.77,"main_claim_p":0.02,"quantitative":false,"quantitative_p":0.03,"role_probabilities":{"gap":0.0,"method":0.04,"result":0.0,"background":0.06,"limitation":0.0,"future_work":0.0,"contribution":0.9,"interpretation":0.0}},{"i":5,"p":0.71,"id":"s5","own":true,"role":"contribution","text":"Twisted and untwisted Cardy boundary states are constructed explicitly and their amplitudes are computed.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.95,"main_claim_p":0.09,"quantitative":false,"quantitative_p":0.07,"role_probabilities":{"gap":0.0,"method":0.02,"result":0.27,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.71,"interpretation":0.0}},{"i":6,"p":0.57,"id":"s6","own":true,"role":"result","text":"In the twisted case we find a perturbative formulation of the model.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.95,"main_claim_p":0.05,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.12,"result":0.57,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.31,"interpretation":0.0}},{"i":7,"p":0.96,"id":"s7","own":true,"role":"method","text":"For this purpose the introduction of an additional fermionic boundary degree of freedom is necessary.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.65,"main_claim_p":0.03,"quantitative":false,"quantitative_p":0.14,"role_probabilities":{"gap":0.0,"method":0.96,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.04,"interpretation":0.0}},{"i":8,"p":0.6,"id":"s8","own":true,"role":"contribution","text":"We compute all bulk one-point functions, bulk-boundary two-point functions and boundary three-point functions.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.95,"main_claim_p":0.07,"quantitative":false,"quantitative_p":0.31,"role_probabilities":{"gap":0.0,"method":0.02,"result":0.38,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.6,"interpretation":0.0}},{"i":9,"p":1.0,"id":"s9","own":true,"role":"result","text":"Logarithmic singularities appear in bulk-boundary as well as pure boundary correlation functions.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.91,"main_claim_p":0.08,"quantitative":false,"quantitative_p":0.07,"role_probabilities":{"gap":0.0,"method":0.0,"result":1.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.0}},{"i":10,"p":0.78,"id":"s10","own":true,"role":"contribution","text":"Finally we turn to world-sheet and target space supersymmetric models.","hedge":{"p":0.5,"label":"asserted"},"own_p":0.71,"main_claim_p":0.03,"quantitative":false,"quantitative_p":0.06,"role_probabilities":{"gap":0.0,"method":0.01,"result":0.0,"background":0.12,"limitation":0.0,"future_work":0.09,"contribution":0.78,"interpretation":0.0}},{"i":11,"p":0.83,"id":"s11","own":false,"role":"background","text":"There is N=2 superconformal symmetry in many supercosets and also in certain supergroups.","hedge":{"p":0.96,"label":"asserted"},"own_p":0.27,"main_claim_p":0.06,"quantitative":false,"quantitative_p":0.46,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.15,"background":0.83,"limitation":0.0,"future_work":0.0,"contribution":0.02,"interpretation":0.0}},{"i":12,"p":0.94,"id":"s12","own":true,"role":"result","text":"In the supergroup case we find some branes that preserve the topological A-twist and some that preserve the B-twist.","hedge":{"p":0.99,"label":"asserted"},"own_p":0.93,"main_claim_p":0.13,"quantitative":false,"quantitative_p":0.13,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.94,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.06,"interpretation":0.0}}]},"compiled":{"main_claim":{"p":0.37,"text":"In the supergroup case we find some branes that preserve the topological A-twist and some that preserve the B-twist.","location":"abstract 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