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Effects of quark-matter symmetry energy on hadron-quark coexistence in neutron-star matter
Nuclear Theory · Submitted 11 Jun 2018
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim As a result, the hadron-quark mixed phase shrinks with only isovector-vector coupling and moves to higher density with isovector-vector and hypercharge-vector couplings.
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The abstract, sentence by sentence
We examine the effects of the isovector-vector coupling and hypercharge-vector coupling in quark matter on hadron-quark coexistence in neutron-star matter. The relativistic mean field theory with the TM1 parameter set and an extended TM1 parameter set are used to describe hadronic matter, and the Nambu-Jona-Lasinio model with scalar, isoscalar-vector, isovector-vector and hypercharge-vector couplings is used to describe deconfined quark matter. The hadron-quark phase transition is constructed via the Gibbs conditions for phase equilibrium. The isovector-vector and hypercharge-vector couplings in quark matter enhance the symmetry energy and hypercharge symmetry energy in neutron-star matter, while their effects are found to be suppressed at high densities by the strange quarks. As a result, the hadron-quark mixed phase shrinks with only isovector-vector coupling and moves to higher density with isovector-vector and hypercharge-vector couplings. The maximum mass of neutron-star increases slightly with isovector-vector and hypercharge-vector couplings.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We examine the effects of the isovector-vector coupling and hypercharge-vector coupling in quark matter on hadron-quark coexistence in neutron-star matter. | contribution 0.99 | 0.89 | 0.07 | unclear 0.51 |
| s1 | The relativistic mean field theory with the TM1 parameter set and an extended TM1 parameter set are used to describe hadronic matter, and the Nambu-Jona-Lasinio model with scalar, isoscalar-vector, isovector-vector and hypercharge-vector couplings is used to describe deconfined quark matter. | method 1.00 | 0.62 | 0.03 | asserted 0.99 |
| s2 | The hadron-quark phase transition is constructed via the Gibbs conditions for phase equilibrium. | method 1.00 | 0.83 | 0.03 | asserted 1.00 |
| s3 | The isovector-vector and hypercharge-vector couplings in quark matter enhance the symmetry energy and hypercharge symmetry energy in neutron-star matter, while their effects are found to be suppressed at high densities by the strange quarks. | result 0.99 | 0.92 | 0.36 | asserted 1.00 |
| s4 | As a result, the hadron-quark mixed phase shrinks with only isovector-vector coupling and moves to higher density with isovector-vector and hypercharge-vector couplings. | result 0.97 | 0.92 | 0.46 | asserted 1.00 |
| s5 | The maximum mass of neutron-star increases slightly with isovector-vector and hypercharge-vector couplings. | result 1.00 | 0.92 | 0.19 | asserted 1.00 |
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The paper
Original abstract
We examine the effects of the isovector-vector coupling and hypercharge-vector coupling in quark matter on hadron-quark coexistence in neutron-star matter. The relativistic mean field theory with the TM1 parameter set and an extended TM1 parameter set are used to describe hadronic matter, and the Nambu-Jona-Lasinio model with scalar, isoscalar-vector, isovector-vector and hypercharge-vector couplings is used to describe deconfined quark matter. The hadron-quark phase transition is constructed via the Gibbs conditions for phase equilibrium. The isovector-vector and hypercharge-vector couplings in quark matter enhance the symmetry energy and hypercharge symmetry energy in neutron-star matter, while their effects are found to be suppressed at high densities by the strange quarks. As a result, the hadron-quark mixed phase shrinks with only isovector-vector coupling and moves to higher density with isovector-vector and hypercharge-vector couplings. The maximum mass of neutron-star increases slightly with isovector-vector and hypercharge-vector couplings.
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References
How the literature uses it
9 arXiv papers cite this in 11 sentences
Papers citing it · 7 sentences without a confident label
Cites it as background 4 papers
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According to literature, the main mechanisms to solve such puzzles are (i) considering the effect of repulsive hyperon-hyperon interaction via exchange of vector mesons [ref] or scalar meson exchange [ref] , (ii) inclusion of repulsive hyperonic three-body forces [ref] , (iii) effect of phase transition from hadronic to deconfined quark matter [ref] , (iv) calculating NS properties with modified/extended theories of gravity [ref] .
Deconfinement of non-strange hadronic matter with nucleons and $\Delta$ baryons to quark matter in neutron stars · Introduction · 0.93
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Apart from the hadron-quark phase transition [ref] or the hyperon-hyperon interaction via exchange of vector mesons [ref] or scalar mesons [ref] , there are many recent paradigm associated with modifications/extensions to the normal General Relativity (GR) theory to resolve the hyperon and the $Δ$ puzzles.
Role of $\Delta$s in determining the properties of Neutron Stars in parameterized hydrostatic equilibrium · Introduction · 0.96
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Quark vector-isoscalar and vector-isovector couplings have been used in the NJL model [ref] , 2-flavor confining QM (CQM) model [ref] , FRG within a quark-meson model [ref] , quark-meson-nucleon (QMN) model [ref] , and bag model [ref] .
GW190814 as a massive rapidly-rotating neutron star with exotic degrees of freedom · Introduction · 0.93
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