{"paper":{"title":"Resonant decay of flat directions","arxiv_id":"hep-ph/0304246","primary_cat":"hep-ph","submitted_at":"2003-04-25T16:05:59+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-1.13-20260917 on the question bank abstract-p1-20260923, exactly as returned. 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case.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.17,"main_claim_p":0.05,"quantitative":false,"quantitative_p":0.49,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.02,"background":0.96,"limitation":0.0,"future_work":0.0,"contribution":0.01,"interpretation":0.01}},{"i":2,"p":0.5,"id":"s2","own":false,"role":"result","text":"The effects of a complex driving field, quartic couplings in the potential, and the presence of a thermal bath are important and cannot be neglected.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.31,"main_claim_p":0.09,"quantitative":false,"quantitative_p":0.04,"role_probabilities":{"gap":0.01,"method":0.05,"result":0.5,"background":0.2,"limitation":0.01,"future_work":0.0,"contribution":0.14,"interpretation":0.09}},{"i":3,"p":0.96,"id":"s3","own":false,"role":"result","text":"Preheating of MSSM flat directions is typically delayed due to out-of-phase oscillations of the real and imaginary components and may be preceded by perturbative decay or $Q$-ball formation.","hedge":{"p":0.83,"label":"hedged_possibility"},"own_p":0.36,"main_claim_p":0.13,"quantitative":false,"quantitative_p":0.08,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.96,"background":0.03,"limitation":0.0,"future_work":0.0,"contribution":0.01,"interpretation":0.0}},{"i":4,"p":0.92,"id":"s4","own":false,"role":"result","text":"Particle production due to the violation of adiabaticity is expected to be inefficient due to back reaction effects.","hedge":{"p":0.85,"label":"hedged_possibility"},"own_p":0.3,"main_claim_p":0.07,"quantitative":false,"quantitative_p":0.09,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.92,"background":0.03,"limitation":0.01,"future_work":0.0,"contribution":0.0,"interpretation":0.04}},{"i":5,"p":0.97,"id":"s5","own":false,"role":"result","text":"For a small initial sneutrino VEV, $<N > \\lesssim m_N/h$ with $m_N$ the mass of the right handed sneutrino and $h$ a yakawa coupling, there are tachyonic instabilities.","hedge":{"p":0.93,"label":"asserted"},"own_p":0.49,"main_claim_p":0.09,"quantitative":true,"quantitative_p":0.97,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.97,"background":0.01,"limitation":0.0,"future_work":0.0,"contribution":0.02,"interpretation":0.0}},{"i":6,"p":0.94,"id":"s6","own":true,"role":"result","text":"The $D$-term quartic couplings do not generate an effective mass for the tachyonic modes, making it an efficient decay channel.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.58,"main_claim_p":0.22,"quantitative":false,"quantitative_p":0.06,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.94,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.06}},{"i":7,"p":0.54,"id":"s7","own":false,"role":"limitation","text":"It is unclear how thermal scattering affects the 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