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arxiv: 1907.05841 · v1 · pith:KBXNDNBPnew · submitted 2019-07-12 · ✦ hep-ph · astro-ph.HE· nucl-th

Compact star properties from an extended linear sigma model

Pith reviewed 2026-05-24 22:18 UTC · model grok-4.3

classification ✦ hep-ph astro-ph.HEnucl-th
keywords compact starsequation of statelinear sigma modelquark mattermass-radius relationvector mesons
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The pith

The equation of state from the axial-vector meson extended linear sigma model produces mass-radius sequences for quark-matter compact stars that meet current observational bounds.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper calculates the mass and radius of compact stars using the pressure-density relation supplied by an effective model of quark matter that includes vector and axial-vector mesons. It checks whether the resulting sequences stay inside the windows allowed by measured neutron-star masses, radii, and tidal deformabilities. The same sequences are placed next to those obtained from simpler versions of the model that omit the vector mesons. The comparison shows how the added mesons shift the maximum mass and the radius at a given mass while still satisfying the astrophysical limits under the assumption that quark matter fills most of the star.

Core claim

When the equation of state is taken from the (axial-)vector meson extended linear sigma model and applied to stars assumed to consist predominantly of quark matter, the computed mass-radius curves remain compatible with existing astrophysical constraints on compact-star masses and radii.

What carries the argument

The equation of state generated by the (axial-)vector meson extended linear sigma model, which supplies the pressure as a function of energy density for quark matter.

If this is right

  • The model can be used to predict further observables such as tidal deformability for binary mergers.
  • The inclusion of vector mesons raises the maximum mass relative to simpler sigma models while still satisfying radius bounds.
  • Direct comparison with simpler models isolates the quantitative effect of the vector-meson terms on the stellar sequence.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • If the quark-matter assumption holds, the same equation of state could be inserted into simulations of neutron-star mergers to test consistency with gravitational-wave data.
  • A hybrid-star construction that adds a thin nuclear crust would shift the radius at low mass but leave the high-mass end largely unchanged.

Load-bearing premise

That most of the star is filled with quark matter.

What would settle it

A precisely measured mass-radius pair for a compact star that lies outside the band of curves produced by this equation of state.

Figures

Figures reproduced from arXiv: 1907.05841 by Gy\"orgy Wolf, J\'anos Tak\'atsy, P\'eter Kov\'acs, Zsolt Sz\'ep.

Figure 1
Figure 1. Figure 1: Left panel: The T = 0 EoS of the eLSM (blue solid line for gv = 0 and blue dashed-dotted line for gv = 2) compared to those of the free constituent quark matter with mass values given in the text (green solid line) and of the Walecka model with (black lines) and without (red lines) including the scalar self-inteaction. For the latter model the dashed-dotted line type indicates that β-equilibrium and charge… view at source ↗
Figure 2
Figure 2. Figure 2: The masses (left panel) and radii (right panel) of the compact stars as functions of the central energy density (ε0). The line style for the different cases correspond to that of [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Mass-radius relations for the eLSM (blue solid line for gv = 0 and blue dashed-dotted line for gv = 2), the free constituent quark matter (green solid line), and the Walecka model for the various cases of [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Left panel: The energy density as a function of radial coordinate inside the maximum mass compact star corresponding to the eLSM with gv = 0. The chiral phase transition occurs at the very edge of the star, hence the whole star is basically composed of chirally symmetric quark matter. Right panel: To ilustrate the effect of the BPS EoS in the Walecka model, we show the pressure as a function of the radial … view at source ↗
Figure 5
Figure 5. Figure 5: M(R) curves of the non-interacting quark model with three different quark mass setups (left curve: mu = md = 322 MeV, ms = 458 MeV, middle curve: mu = md = 75 MeV, ms = 365 MeV and right curve: mu = md = 0 MeV, ms = 90 MeV) compared to the M(R) curve of the eLSM model with gv = 0 in which the quark masses change (rightmost curve). The dashed curves are obtained without imposing the constraints of charge ne… view at source ↗
Figure 6
Figure 6. Figure 6: Dependence of the mass-radius relations on the strength of the Yukawa coupling gv between quarks and the vector meson in the eLSM model. The energy density as a function of radial position is shown in [PITH_FULL_IMAGE:figures/full_fig_p008_6.png] view at source ↗
read the original abstract

The equation of state provided by effective models of strongly interacting matter should comply with the restrictions imposed by current astrophysical observations of compact stars. Using the equation of state given by the (axial-)vector meson extended linear sigma model, we determine the mass-radius relation and study whether these restrictions are satisfied under the assumption that most of the star is filled with quark matter. We also compare the mass-radius sequence with those given by the equations of state of somewhat simpler models.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 2 minor

Summary. The manuscript computes the mass-radius relation for compact stars from the equation of state of an (axial-)vector-meson-extended linear sigma model, under the explicit assumption that most of the star is filled with quark matter, and checks consistency with astrophysical bounds while comparing the resulting sequences to those obtained from simpler models.

Significance. If the central results hold, the work supplies a concrete test of an effective QCD model against compact-star observations; the explicit inclusion of vector mesons in the Lagrangian is a strength that can be directly compared with simpler truncations.

minor comments (2)
  1. The abstract states the quark-matter assumption clearly, so the mass-radius sequences are conditional rather than unconditional predictions; this framing is appropriate and removes the potential circularity concern.
  2. Notation for the model parameters and the precise form of the EoS (e.g., which meson fields are retained) should be introduced once in the main text with a reference to the Lagrangian, to aid readers who wish to reproduce the sequences.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive assessment of our work and the recommendation for minor revision. The manuscript uses the equation of state from the (axial-)vector meson extended linear sigma model to obtain the mass-radius relation for compact stars under the assumption that quark matter dominates the interior, and compares the results to those from simpler models while checking consistency with astrophysical bounds.

Circularity Check

0 steps flagged

No significant circularity identified

full rationale

The derivation starts from the EoS of the (axial-)vector meson extended linear sigma model, applies it to the Tolman-Oppenheimer-Volkoff equation under the explicit assumption that most of the star is quark matter, and produces a mass-radius sequence that is then compared to sequences from simpler models. No step reduces a claimed prediction to a fitted input by construction, no self-citation is invoked as a uniqueness theorem, and the central result remains conditional on the stated assumption rather than being forced by redefinition or parameter renaming. The model inputs are external particle data; the stellar output is a downstream calculation, rendering the chain self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract supplies no information on free parameters, axioms, or invented entities; the model is referred to only by name.

pith-pipeline@v0.9.0 · 5612 in / 1088 out tokens · 24794 ms · 2026-05-24T22:18:55.514609+00:00 · methodology

discussion (0)

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Works this paper leans on

41 extracted references · 41 canonical work pages · 3 internal anchors

  1. [1]

    ALICE Overview

    Grelli, A. ALICE Overview. EPJ Web Conf. 2018, 17, 10100. doi:10.1051/epjconf/201817101005

  2. [2]

    Overview of latest results from PHENIX

    Sakaguchi, T. Overview of latest results from PHENIX. PoS 2019, HardProbes2018, 035. doi:10.22323/1.345.0035

  3. [3]

    The RHIC Beam Energy Scan Phase II: Physics and Upgrades

    Tlusty, D. The RHIC Beam Energy Scan Phase II: Physics and Upgrades. 13th Conference on the Intersections of Particle and Nuclear Physics (CIPANP 2018) Palm Springs, California, USA, May 29-June 3, 2018, [arXiv:nucl-ex/1810.04767]

  4. [4]

    Frontiers of finite temperature lattice QCD

    Borsanyi, S. Frontiers of finite temperature lattice QCD. EPJ Web Conf. 2017, 137, 01006. doi:10.1051/epjconf/201713701006

  5. [5]

    Latest Results from the NA61/SHINE Experiment

    Larsen, D.T. Latest Results from the NA61/SHINE Experiment. KnE Energ. Phys. 2018, 3, 188–194. doi:10.18502/ken.v3i1.1742

  6. [6]

    NICA project at JINR: status and prospects

    Kekelidze, V .D. NICA project at JINR: status and prospects. JINST 2017, 12, C06012. doi:10.1088/1748-0221/12/06/C06012

  7. [7]

    Challenges in QCD matter physics –The scientific programme of the Compressed Baryonic Matter experiment at FAIR

    Ablyazimov, T.; others. Challenges in QCD matter physics –The scientific programme of the Compressed Baryonic Matter experiment at FAIR. Eur. Phys. J. 2017, A53, 60. doi:10.1140/epja/i2017-12248-y

  8. [8]

    Neutron star observations: Prognosis for equation of state constraints

    Lattimer, J.M.; Prakash, M. Neutron star observations: Prognosis for equation of state constraints. Physics Reports 2007, 442, 109–165. doi:10.1016/j.physrep.2007.02.003

  9. [9]

    Colloquium : Measuring the neutron star equation of state using x-ray timing

    Watts, A.L.; others. Colloquium : Measuring the neutron star equation of state using x-ray timing. Rev. Mod. Phys. 2016, 88, 021001. doi:10.1103/RevModPhys.88.021001

  10. [10]

    Critical examination of constraints on the equation of state of dense matter obtained from GW170817

    Tews, I.; Margueron, J.; Reddy, S. Critical examination of constraints on the equation of state of dense matter obtained from GW170817. Phys. Rev. 2018, C98, 045804. doi:10.1103/PhysRevC.98.045804

  11. [11]

    Static Solutions of Einstein’s Field Equations for Spheres of Fluid.Phys

    Tolman, R.C. Static Solutions of Einstein’s Field Equations for Spheres of Fluid.Phys. Rev. 1939, 55, 364–373. doi:10.1103/PhysRev.55.364

  12. [12]

    On Massive Neutron Cores

    Oppenheimer, J.R.; Volkoff, G.M. On Massive Neutron Cores. Phys. Rev. 1939, 55, 374–381. doi:10.1103/PhysRev.55.374

  13. [13]

    A two-solar-mass neutron star measured using Shapiro delay

    Demorest, P .B.; Pennucci, T.; Ransom, S.M.; Roberts, M.S.E.; Hessels, J.W.T. A two-solar-mass neutron star measured using Shapiro delay. Nature 2010, 467, 1081–1083. doi:10.1038/nature09466

  14. [14]

    A Massive Pulsar in a Compact Relativistic Binary

    Antoniadis, J.; Freire, P .C.C.; Wex, N.; Tauris, T.M.; Lynch, R.S.; van Kerkwijk, M.H.; Kramer, M.; Bassa, C.; Dhillon, V .S.; Driebe, T.; Hessels, J.W.T.; Kaspi, V .M.; Kondratiev, V .I.; Langer, N.; Marsh, T.R.; McLaughlin, M.A.; Pennucci, T.T.; Ransom, S.M.; Stairs, I.H.; van Leeuwen, J.; Verbiest, J.P .W.; Whelan, D.G. A Massive Pulsar in a Compact R...

  15. [15]

    Dense baryonic matter: constraints from recent neutron star observations

    Hell, T.; Weise, W. Dense baryonic matter: constraints from recent neutron star observations. Phys. Rev. 2014, C90, 045801. doi:10.1103/PhysRevC.90.045801

  16. [16]

    Neutron star masses and radii from quiescent low-mass X-ray binaries

    Lattimer, J.M.; Steiner, A.W. Neutron star masses and radii from quiescent low-mass X-ray binaries. The Astrophysical Journal 2014, 784, 123. doi:10.1088/0004-637x/784/2/123. Universe 2019, xx, 5 10 of 11

  17. [17]

    Bayesian Analysis for Extracting Properties of the Nuclear Equation of State from Observational Data including Tidal Deformability from GW170817

    Ayriyan, A.; Alvarez-Castillo, D.; Blaschke, D.; Grigorian, H. Bayesian Analysis for Extracting Properties of the Nuclear Equation of State from Observational Data including Tidal Deformability from GW170817. Universe 2019, 5, 61. doi:10.3390/universe5020061

  18. [18]

    New constraints on radii and tidal deformabilities of neutron stars from GW170817

    Most, E.R.; Weih, L.R.; Rezzolla, L.; Schaffner-Bielich, J. New constraints on radii and tidal deformabilities of neutron stars from GW170817. Phys. Rev. Lett. 2018, 120, 261103. doi:10.1103/PhysRevLett.120.261103

  19. [19]

    GW170817: Measurements of Neutron Star Radii and Equation of State

    Abbott, B.P .; Abbott, R.; Abbott, T.D.; Acernese, F.; Ackley, K.; Adams, C.; Adams, T.; Addesso, P .; Adhikari, R.X.; Adya, V .B.; et al.. GW170817: Measurements of Neutron Star Radii and Equation of State. Physical Review Letters 2018, 121, 161101. doi:10.1103/PhysRevLett.121.161101

  20. [20]

    Constraining the neutron star equation of state using Pulse Profile Modeling

    Watts, A.L. Constraining the neutron star equation of state using Pulse Profile Modeling. Xiamen- CUSTIPEN Workshop on the EOS of Dense Neutron-Rich Matter in the Era of Gravitational Wave Astronomy Xiamen, China, January 3-7, 2019, 2019, [arXiv:astro-ph.HE/1904.07012]

  21. [21]

    Existence of the critical endpoint in the vector meson extended linear sigma model

    Kovács, P .; Szép, Z.; Wolf, G. Existence of the critical endpoint in the vector meson extended linear sigma model. Phys. Rev. 2016, D93, 114014. doi:10.1103/PhysRevD.93.114014

  22. [22]

    Meson vacuum phenomenology in a three-flavor linear sigma model with (axial-)vector mesons

    Parganlija, D.; Kovács, P .; Wolf, G.; Giacosa, F.; Rischke, D.H. Meson vacuum phenomenology in a three-flavor linear sigma model with (axial-)vector mesons. Phys. Rev. 2013, D87, 014011. doi:10.1103/PhysRevD.87.014011

  23. [23]

    Compact stars in a SU(3) Quark-Meson Model

    Zacchi, A.; Stiele, R.; Schaffner-Bielich, J. Compact stars in a SU(3) Quark-Meson Model. Phys. Rev. 2015, D92, 045022. doi:10.1103/PhysRevD.92.045022

  24. [24]

    Heavy hybrid stars from multi-quark interactions

    Benic, S. Heavy hybrid stars from multi-quark interactions. Eur. Phys. J. 2014, A50, 111. doi:10.1140/epja/i2014-14111-1

  25. [25]

    A new quark-hadron hybrid equation of state for astrophysics - I

    Benic, S.; Blaschke, D.; Alvarez-Castillo, D.E.; Fischer, T.; Typel, S. A new quark-hadron hybrid equation of state for astrophysics - I. High-mass twin compact stars. Astron. Astrophys. 2015, 577, A40. doi:10.1051/0004-6361/201425318

  26. [26]

    Constraining the properties of neutron-star matter with observations

    Annala, E.; Gorda, T.; Kurkela, A.; Nättilä, J.; Vuorinen, A. Constraining the properties of neutron-star matter with observations. 12th INTEGRAL conference and 1st AHEAD Gamma-ray workshop (INTEGRAL 2019): INTEGRAL looks AHEAD to Multi-Messenger Astrophysics Geneva, Switzerland, February 11-15, 2019, 2019, [arXiv:astro-ph.HE/1904.01354]

  27. [27]

    A theory of highly condensed matter

    Walecka, J.D. A theory of highly condensed matter. Annals of Physics 1974, 83, 491–529. doi:10.1016/0003-4916(74)90208-5

  28. [28]

    Review of Particle Physics

    Patrignani, C.; et al. Review of Particle Physics. Chin. Phys. 2016, C40, 100001. doi:10.1088/1674-1137/40/10/100001

  29. [29]

    James, M

    James, F.; Roos, M. Minuit - a system for function minimization and analysis of the parameter errors and correlations. Computer Physics Communications 1975, 10, 343 – 367. doi:10.1016/0010-4655(75)90039-9

  30. [30]

    The QCD transition temperature: Results with physical masses in the continuum limit

    Aoki, Y.; Fodor, Z.; Katz, S.; Szabó, K. The QCD transition temperature: Results with physical masses in the continuum limit. Physics Letters B 2006, 643, 46 – 54. doi:10.1016/j.physletb.2006.10.021

  31. [31]

    The chiral and deconfinement aspects of the QCD transition

    Bazavov, A.; others. The chiral and deconfinement aspects of the QCD transition. Phys. Rev. 2012, D85, 054503. doi:10.1103/PhysRevD.85.054503

  32. [32]

    Properties of hot and dense strongly interacting matter

    Almási, G. Properties of hot and dense strongly interacting matter. PhD thesis, Technische Universität, Darmstadt, 2017. http://tuprints.ulb.tu-darmstadt.de/6748/

  33. [33]

    Dense matter in compact stars: A pedagogical introduction ; Vol

    Schmitt, A. Dense matter in compact stars: A pedagogical introduction ; Vol. 811, Lecture Notes in Physics , Springer, Berlin, 2010; pp. 1–111. doi:10.1007/978-3-642-12866-0

  34. [34]

    Compact Stars: Nuclear Physics, Particle Physics, and General Relativity , 2nd ed.; Astronomy and Astrophysics Library, Springer, New York, 2000

    Glendenning, N. Compact Stars: Nuclear Physics, Particle Physics, and General Relativity , 2nd ed.; Astronomy and Astrophysics Library, Springer, New York, 2000

  35. [35]

    Symmetry energy, its density slope, and neutron-proton effective mass splitting at normal density extracted from global nucleon optical potentials

    Xu, C.; Li, B.A.; Chen, L.W. Symmetry energy, its density slope, and neutron-proton effective mass splitting at normal density extracted from global nucleon optical potentials. Phys. Rev. 2010, C82, 054607. doi:10.1103/PhysRevC.82.054607

  36. [36]

    Estimating the variation of neutron star observables by symmetric dense nuclear matter properties

    Pósfay, P .; Barnaföldi, G.G.; Jakovác, A. Estimating the variation of neutron star observables by symmetric dense nuclear matter properties. [arXiv:hep-ph/1905.01872]

  37. [37]

    The Ground state of matter at high densities: Equation of state and stellar models

    Baym, G.; Pethick, C.; Sutherland, P . The Ground state of matter at high densities: Equation of state and stellar models. Astrophys. J. 1971, 170, 299–317. doi:10.1086/151216

  38. [38]

    Neutron star radii and crusts: uncertainties and unified equations of state

    Fortin, M.; Providencia, C.; Raduta, A.R.; Gulminelli, F.; Zdunik, J.L.; Haensel, P .; Bejger, M. Neutron star radii and crusts: uncertainties and unified equations of state. Phys. Rev. 2016, C94, 035804. doi:10.1103/PhysRevC.94.035804. Universe 2019, xx, 5 11 of 11

  39. [39]

    Phases of dense matter in compact stars

    Blaschke, D.; Chamel, N. Phases of dense matter in compact stars. Astrophys. Space Sci. Libr. 2018, 457, 337–400. doi:10.1007/978-3-319-97616-7_7

  40. [40]

    Analytical representations of unified equations of state for neutron-star matter

    Potekhin, A.Y.; Fantina, A.F.; Chamel, N.; Pearson, J.M.; Goriely, S. Analytical representations of unified equations of state for neutron-star matter. Astron. Astrophys. 2013, 560, A48. doi:10.1051/0004-6361/201321697

  41. [41]

    A Radio Pulsar Spinning at 716 Hz

    Hessels, J.W.T.; Ransom, S.M.; Stairs, I.H.; Freire, P .C.C.; Kaspi, V .M.; Camilo, F. A Radio Pulsar Spinning at 716 Hz. Science 2006, 311, 1901–1904. doi:10.1126/science.1123430. c⃝ 2019 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution...