{"paper":{"title":"Anatomy of Null Contractions","arxiv_id":"2406.15061","primary_cat":"hep-th","submitted_at":"2024-06-21T11:25:44+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-1.13.0 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 v1","sentences":[{"i":0,"p":1.0,"id":"s0","own":true,"role":"contribution","text":"We introduce null contractions of the Poincare and relativistic conformal algebras.","hedge":{"p":0.99,"label":"asserted"},"own_p":0.94,"main_claim_p":0.12,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":1.0,"interpretation":0.0}},{"i":1,"p":0.95,"id":"s1","own":true,"role":"method","text":"The longitudinal null contraction involves writing the algebra in lightcone coordinates and contracting one of the null directions.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.58,"main_claim_p":0.05,"quantitative":false,"quantitative_p":0.11,"role_probabilities":{"gap":0.0,"method":0.95,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.05,"interpretation":0.0}},{"i":2,"p":1.0,"id":"s2","own":true,"role":"result","text":"For the Poincare algebra, this yields two non-overlapping co-dimension one Carroll algebras.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.88,"main_claim_p":0.19,"quantitative":true,"quantitative_p":0.78,"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":3,"p":0.77,"id":"s3","own":true,"role":"result","text":"The transverse contraction is a limit on the spatial dimensions and yields two non-overlapping co-dimension one Galilean algebras.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.82,"main_claim_p":0.12,"quantitative":true,"quantitative_p":0.65,"role_probabilities":{"gap":0.0,"method":0.13,"result":0.77,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.1,"interpretation":0.0}},{"i":4,"p":0.84,"id":"s4","own":true,"role":"result","text":"We find, similar to Susskind's original observation of the non-relativistic case, that the Poincare algebra, written in the lightcone coordinates, naturally contains Carrollian sub-algebras in one lower dimension.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.69,"main_claim_p":0.3,"quantitative":true,"quantitative_p":0.51,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.84,"background":0.04,"limitation":0.0,"future_work":0.0,"contribution":0.01,"interpretation":0.11}},{"i":5,"p":0.76,"id":"s5","own":true,"role":"interpretation","text":"The effect of the longitudinal contraction, which essentially focusses on the null direction, is to disentangle the two Carroll algebras that now correspond to the symmetries of the two null boundaries.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.78,"main_claim_p":0.18,"quantitative":false,"quantitative_p":0.25,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.24,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.76}},{"i":6,"p":0.67,"id":"s6","own":true,"role":"result","text":"The transverse contraction similarly separates the overlapping Galilean sub-algebras of the original Poincare algebra.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.79,"main_claim_p":0.1,"quantitative":false,"quantitative_p":0.13,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.67,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.01,"interpretation":0.32}},{"i":7,"p":0.59,"id":"s7","own":true,"role":"contribution","text":"We discuss aspects of the conformal case, where we get lower dimensional Carroll Conformal algebras and Schrodinger 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