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Quark Matter
High Energy Physics - Phenomenology · Submitted 30 Apr 2003
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The main part of these lectures is devoted to the phenomenon of color superconductivity.
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The abstract, sentence by sentence
In these lectures we provide an introduction to the theory of QCD at very high baryon density. We begin with a review of some aspects of quantum many-body system that are relevant in the QCD context. We also provide a brief review of QCD and its symmetries. The main part of these lectures is devoted to the phenomenon of color superconductivity. We discuss the use of weak coupling methods and study the phase structure as a function of the number of flavors and their masses. We also introduce effective theories that describe low energy excitations at high baryon density. Finally, we use effective field theory methods in order to study the effects of a non-zero strange quark mass.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In these lectures we provide an introduction to the theory of QCD at very high baryon density. | contribution 0.84 | 0.64 | 0.04 | asserted 0.76 |
| s1 | We begin with a review of some aspects of quantum many-body system that are relevant in the QCD context. | background 0.87 | 0.37 | 0.02 | asserted 0.75 |
| s2 | We also provide a brief review of QCD and its symmetries. | background 0.94 | 0.43 | 0.02 | asserted 0.76 |
| s3 | The main part of these lectures is devoted to the phenomenon of color superconductivity. | contribution 0.96 | 0.42 | 0.09 | asserted 0.94 |
| s4 | We discuss the use of weak coupling methods and study the phase structure as a function of the number of flavors and their masses. | contribution 0.55 | 0.71 | 0.05 | asserted 0.88 |
| s5 | We also introduce effective theories that describe low energy excitations at high baryon density. | contribution 0.63 | 0.70 | 0.03 | asserted 0.97 |
| s6 | Finally, we use effective field theory methods in order to study the effects of a non-zero strange quark mass. | contribution 0.53 | 0.81 | 0.05 | asserted 0.97 |
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The paper
Original abstract
In these lectures we provide an introduction to the theory of QCD at very high baryon density. We begin with a review of some aspects of quantum many-body system that are relevant in the QCD context. We also provide a brief review of QCD and its symmetries. The main part of these lectures is devoted to the phenomenon of color superconductivity. We discuss the use of weak coupling methods and study the phase structure as a function of the number of flavors and their masses. We also introduce effective theories that describe low energy excitations at high baryon density. Finally, we use effective field theory methods in order to study the effects of a non-zero strange quark mass.
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References
How the literature uses it
16 arXiv papers cite this in 16 sentences
Papers citing it · 3 sentences without a confident label
Cites it as background 13 papers
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There, quarks form Cooper pairs which condense as color superconductors [ref] .
Dyson-Schwinger approach to color superconductivity at finite temperature and density · Introduction · 0.90
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At high densities and low temperatures, on the other hand, strongly interacting matter is expected to be a color superconductor, where the quarks form Cooper pairs (for reviews, see [ref] ).
Role of two-flavor color superconductor pairing in a three-flavor Nambu--Jona-Lasinio model with axial anomaly · Introduction · 1.00
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In the regime of strong interaction where quarks and gluons are elementary particles described by quantum chromodynamics (QCD), a similar phenomena, the so called color superconductivity was first proposed in cold dense quark matter by Barrois [ref] , Bailin and Love [ref] , and further developed by many others (for reviews, see [ref] ).
Some aspects of color superconductivity: an introduction · What is color superconductivity? · 0.99
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