{"paper":{"title":"N=4 Super Yang-Mills Plasma","arxiv_id":"1203.1856","primary_cat":"hep-th","submitted_at":"2012-03-08T17:25:55+00:00","version_compiled":"v4"},"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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discussed.","hedge":{"p":0.81,"label":"asserted"},"own_p":0.62,"main_claim_p":0.02,"quantitative":false,"quantitative_p":0.03,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.0,"background":0.03,"limitation":0.0,"future_work":0.0,"contribution":0.97,"interpretation":0.0}},{"i":2,"p":0.94,"id":"s2","own":true,"role":"method","text":"Since the Keldysh-Schwinger approach is used, the collective excitations in both equilibrium and non-equilibrium plasma are under consideration.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.59,"main_claim_p":0.03,"quantitative":false,"quantitative_p":0.06,"role_probabilities":{"gap":0.0,"method":0.94,"result":0.0,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.06,"interpretation":0.0}},{"i":3,"p":0.44,"id":"s3","own":true,"role":"contribution","text":"The dispersion equations of gluon, fermion, and scalar modes are written down and the self-energies, which enter the equations, are computed in the Hard Loop Approximation.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.91,"main_claim_p":0.04,"quantitative":false,"quantitative_p":0.09,"role_probabilities":{"gap":0.0,"method":0.37,"result":0.19,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.44,"interpretation":0.0}},{"i":4,"p":0.59,"id":"s4","own":true,"role":"contribution","text":"The self-energies are discussed in the context of effective action which is also given.","hedge":{"p":0.99,"label":"asserted"},"own_p":0.82,"main_claim_p":0.02,"quantitative":false,"quantitative_p":0.03,"role_probabilities":{"gap":0.0,"method":0.28,"result":0.11,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.59,"interpretation":0.02}},{"i":5,"p":0.88,"id":"s5","own":true,"role":"result","text":"The gluon modes and fermion ones appear to be the same as those in the QCD plasma of gluons and massless quarks.","hedge":{"p":0.62,"label":"asserted"},"own_p":0.77,"main_claim_p":0.11,"quantitative":true,"quantitative_p":0.72,"role_probabilities":{"gap":0.0,"method":0.0,"result":0.88,"background":0.0,"limitation":0.0,"future_work":0.0,"contribution":0.0,"interpretation":0.12}},{"i":6,"p":0.99,"id":"s6","own":true,"role":"result","text":"The scalar modes are as of a free relativistic massive particle.","hedge":{"p":1.0,"label":"asserted"},"own_p":0.8,"main_claim_p":0.05,"quantitative":false,"quantitative_p":0.14,"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":0.89,"id":"s7","own":true,"role":"contribution","text":"The binary collisional processes, which occur at the lowest nontrivial order of the coupling constant, are reviewed and then the transport properties of the plasma are 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