{"arxiv_id":"hep-ph/0404164","incoming":{"papers":41,"sentences":49,"groups":[{"kind":"background","label":"Cites it as background","papers":17,"sentences":18,"quotes":[{"arxiv_id":"2102.11145","title":"Robust approach to thermal resummation: Standard Model meets a singlet","url":"/paper/2102.11145","section":"Dimensional reduction for a high-temperature 3d effective theory","sentence":"In the context of electroweak theories, classic references are [ref] but we also refer [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1310.5629","title":"Gluon screening mass at finite temperature from Landau gauge gluon propagator in lattice QCD","url":"/paper/1310.5629","section":"Introduction","sentence":"Above the deconfinement temperature of QCD, finite temperature field theory, see e.g. [ref] , treats the gluons as an ideal gas of massive particles.","intent_p":0.95,"contests_p":null},{"arxiv_id":"2310.02308","title":"Higher orders for cosmological phase transitions: a global study in a Yukawa model","url":"/paper/2310.02308","section":"Dimensional reduction","sentence":"Thus one can view the equilibrium thermodynamics of the four dimensional (4d) theory as the vacuum dynamics of infinitely many 3d fields [ref] , the fields $φ_n$ with effective squared masses $m_n^2 = m^2 + (2 πT n)^2$ and the fields $_n$ with effective squared masses $m_ψ^2 + (2πT (n+1))^2$.","intent_p":0.83,"contests_p":null},{"arxiv_id":"1801.00863","title":"Parton self-energies for general momentum-space anisotropy","url":"/paper/1801.00863","section":"Introduction","sentence":"As a result, the current theoretical understanding of QGP is mostly based on lattice QCD [ref] , hard-(thermal)-loop perturbation theory [ref] , effective hydrodynamic models [ref] , AdS/CFT inspired dual descriptions of the QGP [ref] , etc.","intent_p":0.93,"contests_p":null},{"arxiv_id":"2401.08384","title":"Shear and bulk viscosity of quark-gluon plasma with Gribov gluons and quasiparticle quarks","url":"/paper/2401.08384","section":"Introduction","sentence":"The transport properties of the QGP have also been extensively studied in the high-temperature regime using resummed perturbation theory [ref] as well as lattice calculations [ref] .","intent_p":0.83,"contests_p":null}]}],"unlabelled_sentences":31},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/hep-ph/0404164"}}