{"paper":{"title":"Post-Inflationary Curvature Perturbations","arxiv_id":"astro-ph/0401407","primary_cat":"astro-ph","submitted_at":"2004-01-20T21:46:03+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. 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scenarios.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.24,"main_claim_p":0.09,"quantitative":false,"quantitative_p":0.16,"role_probabilities":{"gap":0.0,"method":0.14,"result":0.04,"background":0.53,"limitation":0.0,"future_work":0.0,"contribution":0.18,"interpretation":0.11}},{"i":2,"p":0.72,"id":"s2","own":false,"role":"background","text":"During inflation, the trajectory along which the fields are rolling down will fluctuate.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.17,"main_claim_p":0.03,"quantitative":false,"quantitative_p":0.03,"role_probabilities":{"gap":0.0,"method":0.22,"result":0.01,"background":0.72,"limitation":0.0,"future_work":0.0,"contribution":0.03,"interpretation":0.02}},{"i":3,"p":0.44,"id":"s3","own":false,"role":"method","text":"When inflation ends, the fields enter the oscillatory phase along different directions in different parts of the universe.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.27,"main_claim_p":0.03,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.0,"method":0.44,"result":0.09,"background":0.28,"limitation":0.0,"future_work":0.0,"contribution":0.1,"interpretation":0.09}},{"i":4,"p":0.59,"id":"s4","own":false,"role":"interpretation","text":"Different oscillatory trajectories can have different effective equations of state and reheating rates, so that different parts of the universe will evolve differently.","hedge":{"p":0.73,"label":"asserted"},"own_p":0.39,"main_claim_p":0.07,"quantitative":false,"quantitative_p":0.07,"role_probabilities":{"gap":0.0,"method":0.24,"result":0.1,"background":0.02,"limitation":0.0,"future_work":0.0,"contribution":0.05,"interpretation":0.59}},{"i":5,"p":0.58,"id":"s5","own":false,"role":"interpretation","text":"This translates the isocurvature perturbations into the curvature perturbations.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.39,"main_claim_p":0.13,"quantitative":false,"quantitative_p":0.03,"role_probabilities":{"gap":0.0,"method":0.25,"result":0.14,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.03,"interpretation":0.58}},{"i":6,"p":0.99,"id":"s6","own":true,"role":"result","text":"If all light fields make similar contributions to the potential energy, the postinflationary curvature perturbations are much smaller than the standard inflationary curvature perturbations.","hedge":{"p":0.97,"label":"asserted"},"own_p":0.66,"main_claim_p":0.14,"quantitative":true,"quantitative_p":0.97,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.99,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.01}},{"i":7,"p":0.98,"id":"s7","own":true,"role":"result","text":"But if different light fields make very different contributions to the potential energy, the postinflationary curvature perturbations can exceed the inflationary perturbations.","hedge":{"p":0.98,"label":"hedged_possibility"},"own_p":0.61,"main_claim_p":0.26,"quantitative":true,"quantitative_p":0.95,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.98,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.02}},{"i":8,"p":0.97,"id":"s8","own":true,"role":"result","text":"The characteristic feature of postinflationary perturbations is non-Gaussianity $\\sim \\pm 1$.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.69,"main_claim_p":0.31,"quantitative":true,"quantitative_p":0.93,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.97,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.03}}]},"compiled":{"main_claim":{"p":0.5,"text":"The characteristic feature of postinflationary perturbations is non-Gaussianity $\\sim \\pm 1$.","location":"abstract s8","hedge_strength":{"p":1.0,"label":"asserted"}},"provenance":{"route":{"via":"TypeSafe 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