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Dyson-Schwinger equations towards cold-dense QCD matter with improved truncations
High Energy Physics - Phenomenology · Submitted 25 Oct 2023
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The result shows that our modified scheme can not only describe the phase transition of the cold dense matter well but also the deduced equation of state of the matter can describe the recent astronomical observations consistently.
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The abstract, sentence by sentence
We take the Dyson-Schwinger equation (DSE) approach of QCD to study the phase transition and the equation of state of cold dense matter. Besides the bare vertex and Gauss gluon model, we take into account an improved truncation scheme, the CLRQ vertex and infrared-constant gluon model. For the dynamical chiral symmetry breaking solution of the DSE, we require that the emergence of quark number density to be at the chemical potential for the nuclear liquid-gas phase transition to take place, by incorporating a chemical potential dependent modification factor to the gluon model. The result shows that our modified scheme can not only describe the phase transition of the cold dense matter well but also the deduced equation of state of the matter can describe the recent astronomical observations consistently.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We take the Dyson-Schwinger equation (DSE) approach of QCD to study the phase transition and the equation of state of cold dense matter. | contribution 0.90 | 0.89 | 0.03 | asserted 0.74 |
| s1 | Besides the bare vertex and Gauss gluon model, we take into account an improved truncation scheme, the CLRQ vertex and infrared-constant gluon model. | method 0.92 | 0.86 | 0.02 | asserted 0.98 |
| s2 | For the dynamical chiral symmetry breaking solution of the DSE, we require that the emergence of quark number density to be at the chemical potential for the nuclear liquid-gas phase transition to take place, by incorporating a chemical potential dependent modification factor to the gluon model. | method 0.97 | 0.86 | 0.05 | asserted 0.96 |
| s3 | The result shows that our modified scheme can not only describe the phase transition of the cold dense matter well but also the deduced equation of state of the matter can describe the recent astronomical observations consistently. | result 0.94 | 0.95 | 0.91 | asserted 0.96 |
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The paper
Original abstract
We take the Dyson-Schwinger equation (DSE) approach of QCD to study the phase transition and the equation of state of cold dense matter. Besides the bare vertex and Gauss gluon model, we take into account an improved truncation scheme, the CLRQ vertex and infrared-constant gluon model. For the dynamical chiral symmetry breaking solution of the DSE, we require that the emergence of quark number density to be at the chemical potential for the nuclear liquid-gas phase transition to take place, by incorporating a chemical potential dependent modification factor to the gluon model. The result shows that our modified scheme can not only describe the phase transition of the cold dense matter well but also the deduced equation of state of the matter can describe the recent astronomical observations consistently.
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What this paper does with the arXiv papers it cites
What it cites · 118 sentences without a confident label
Uses the method or tool of 2 papers
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For the modification function $h(μ_q)$, we follow our previous work [ref] : [equation] where $μ_q,c=923/3$MeV is the quark chemical potential corresponding to the nuclear liquid-gas phase transition, $β$ is a parameter to be fixed.
QCD phase transition and equation of state of stellar strong interaction matter via Dyson-Schwinger equation approach · Modification to truncation scheme · 0.89
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After solving the gap equation at some quark chemical potential, the number density of quarks can be obtained through [ref] :
Chemical potential and the gap equation · Emergence of quark number and comparison of the schemes · 0.97
Uses data or values from 1 paper
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In this paper, we take $η=0.65$ as that in Ref. [ref] .
QCD phase transitions via a refined truncation of Dyson-Schwinger equations · Dyson-Schwinger equation approach · 0.99
Cites as support 3 papers
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However, both the mass function and the chiral susceptibility ($∂B/∂m_q^$) are negative in small chemical potential region (see, e.g. Ref. [ref] ), and it has been proved that the negative chiral susceptibility corresponds to an unstable phase [ref] .
Phase diagram and critical endpoint for strongly-interacting quarks · Isosymmetric phase transition and coexistence region · 0.97
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However, both the mass function and the chiral susceptibility ($∂B/∂m_q^$) are negative in small chemical potential region (see, e.g. Ref. [ref] ), and it has been proved that the negative chiral susceptibility corresponds to an unstable phase [ref] .
Interaction model for the gap equation · Isosymmetric phase transition and coexistence region · 0.97
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However, both the mass function and the chiral susceptibility ($∂B/∂m_q^$) are negative in small chemical potential region (see, e.g. Ref. [ref] ), and it has been proved that the negative chiral susceptibility corresponds to an unstable phase [ref] .
QCD phase transitions via a refined truncation of Dyson-Schwinger equations · Isosymmetric phase transition and coexistence region · 0.97
Cites as background 33 papers
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The DSE approach has also been taken to study the cold dense matter [ref] , which is relevant in neutron stars.
Chemical potential and the gap equation · Introduction · 0.93
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The DSE approach has also been taken to study the cold dense matter [ref] , which is relevant in neutron stars.
Hybrid stars with the Dyson-Schwinger quark model · Introduction · 0.93
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The DSE approach has also been taken to study the cold dense matter [ref] , which is relevant in neutron stars.
Hybrid protoneutron stars with the Dyson-Schwinger quark model · Introduction · 0.93
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