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Hard Thermal Loops in a Moving Plasma and a Magnetic Mass Term
High Energy Physics - Theory · Submitted 13 Jun 1994
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Generalizing from this we suggest a candidate for the magnetic mass term.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
We consider the hard thermal loops of QCD for a moving quark-gluon plasma. Generalizing from this we suggest a candidate for the magnetic mass term. This term may also be useful in understanding the mass gap of three-dimensional non-Abelian gauge theories.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider the hard thermal loops of QCD for a moving quark-gluon plasma. | contribution 0.88 | 0.76 | 0.05 | asserted 0.77 |
| s1 | Generalizing from this we suggest a candidate for the magnetic mass term. | contribution 0.78 | 0.54 | 0.55 | hedged possibility 0.98 |
| s2 | This term may also be useful in understanding the mass gap of three-dimensional non-Abelian gauge theories. | interpretation 0.89 | 0.18 | 0.16 | hedged possibility 1.00 |
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The paper
Original abstract
We consider the hard thermal loops of QCD for a moving quark-gluon plasma. Generalizing from this we suggest a candidate for the magnetic mass term. This term may also be useful in understanding the mass gap of three-dimensional non-Abelian gauge theories.
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How the literature uses it
3 arXiv papers cite this in 10 sentences
Papers citing it · 9 sentences without a confident label
Cites it as background 1 paper
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We begin with a brief review of the mass-term introduced in [ref] and its various relevant algebraic properties.
A Supersymmetry Preserving Mass-Deformation of N=1 Super Yang-Mills in D=2+1 · Introduction · 0.91
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