pith. sign in

arxiv: 1907.03283 · v1 · pith:MCD5EJEInew · submitted 2019-07-07 · ⚛️ nucl-th · astro-ph.HE· astro-ph.SR

Constraints from the GW170817 merger event on the nuclear matter equation of state

Pith reviewed 2026-05-25 01:22 UTC · model grok-4.3

classification ⚛️ nucl-th astro-ph.HEastro-ph.SR
keywords GW170817neutron starequation of statetidal deformabilitynuclear matterhybrid starsmoment of inertiaradius constraint
0
0 comments X

The pith

The GW170817 merger constrains neutron star radii to 12-13 km and selects compatible microscopic equations of state.

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

The paper compares the pressure-density relation extracted from the GW170817 neutron star merger with results from heavy-ion collisions. It computes neutron star moment of inertia and tidal deformability for a set of microscopic equations of state that describe both nuclear and hybrid star configurations, and verifies that several universal relations hold across these models. The resulting radius range of 12-13 km is compatible with the merger signal, thereby identifying which equations of state remain viable.

Core claim

Calculations with microscopic equations of state for nuclear and hybrid stars show that the GW170817 event implies neutron star radii between 12 and 13 kilometers, which selects the equations of state consistent with both the merger data and the pressure-density behavior observed in heavy-ion collisions while confirming universal relations among moment of inertia, tidal deformability, and other global properties.

What carries the argument

Microscopic equations of state for nuclear and hybrid configurations, used to compute tidal deformability and moment of inertia under the densities realized in neutron stars.

If this is right

  • Equations of state that produce radii outside 12-13 km are excluded by the merger constraints.
  • The pressure-density curves favored by the merger overlap with those extracted from heavy-ion collision data.
  • Universal relations between moment of inertia, tidal deformability, and compactness continue to hold for the retained nuclear and hybrid models.
  • Both purely nuclear and hybrid configurations with quark cores remain possible if they satisfy the radius window.

Where Pith is reading between the lines

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

  • Repeated gravitational-wave detections of mergers could tighten the radius window and further discriminate among the surviving equations of state.
  • The 12-13 km range supplies an independent anchor that can be combined with x-ray radius measurements or pulsar timing data to test the same equations of state.
  • If hybrid stars are realized, the transition density to quark matter must lie such that the overall radius still falls inside the observed interval.

Load-bearing premise

The chosen microscopic equations of state remain accurate when extrapolated to the high densities and neutron-proton asymmetries inside neutron stars.

What would settle it

A radius measurement for a neutron star that lies clearly outside the 12-13 km interval would rule out the equations of state identified as compatible.

Figures

Figures reproduced from arXiv: 1907.03283 by A. Figura, G. F. Burgio, H.-J. Schulze, INFN Sezione di Catania), J.-B. Wei (Dipartimento di Fisica e Astronomia, Universita' di Catania.

Figure 1
Figure 1. Figure 1: Pressure vs. density of symmetric nuclear matter for different EOSs in comparison with the phe￾nomenological constraints from heavy ion collisions (brown and yellow shaded areas), and from GW170817 (blue shaded area). ρ0 = 0.16 fm−3 is the saturation density. exploring the EOS and its incompressibility. In Ref. [47] the flow and kaon production analysis was summarized by plotting the region in the pressure… view at source ↗
Figure 2
Figure 2. Figure 2: (Left panel) Mass-radius relations for different EOSs. Solid (dotted) curves are plotted for micro￾scopic (phenomenological) EOSs. Dashed and dot-dashed curves display hybrid stars in the DSM approach with DS1 and DS2, respectively. Open circles indicate the values of the maximum mass. The shaded areas show limits derived in [51]. (Right panel) Correlations between M, R, and Λ for a single NS with differen… view at source ↗
Figure 3
Figure 3. Figure 3: I/M3 (left panel) and I/MR2 (right panel) vs. β = M/R for 10+4 different nucleonic+hybrid EOSs. The lower panels show the fractional deviations from the fit curves. the mass and the moment of inertia of the NS is known [7, 73]. Below we discuss some of those relations. For details the reader is referred to Ref. [74]. In [PITH_FULL_IMAGE:figures/full_fig_p007_3.png] view at source ↗
read the original abstract

The detection of the GW170817 neutron star merger event has incited an intense research activity towards the understanding of the nuclear matter equation of state. In this paper we compare in particular the pressure-density relation obtained from heavy-ion collisions with the analysis of the NS merger event. Moreover, we present recent calculations of neutron star's moment of inertia and tidal deformability using various microscopic equations of state for nuclear and hybrid star configurations, and confirm several universal relations. We also discuss the recent constraints for the NS radii determined by GW170817, and find compatible radii between 12 and 13 kilometers, thus identifying the suitable equations of state.

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

1 major / 0 minor

Summary. The manuscript compares the pressure-density relation from heavy-ion collisions with constraints inferred from the GW170817 neutron-star merger. It reports calculations of neutron-star moment of inertia and tidal deformability for a set of microscopic nuclear and hybrid equations of state, confirms several universal relations, and concludes that radii in the range 12–13 km are compatible with the event, thereby identifying suitable equations of state.

Significance. If the radius constraint and the underlying EOS extrapolations hold, the work supplies a concrete link between laboratory heavy-ion data and multi-messenger astrophysics, narrowing the set of viable microscopic models for dense matter.

major comments (1)
  1. [Abstract] Abstract (paragraph on calculations of moment of inertia and tidal deformability): the central claim that radii of 12–13 km are compatible with GW170817 and thereby identify suitable EOS rests on the assumption that the employed microscopic EOS remain accurate when extrapolated to the densities (~2–5 ρ_sat) and β-equilibrium asymmetries realized in neutron stars. The manuscript compares the pressure-density relation only to heavy-ion data at lower densities and different isospin; no independent cross-check (e.g., maximum-mass consistency or other NS observables independent of the same models) is described that would validate the extrapolation step itself.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the constructive comments. We address the major comment on the extrapolation of the microscopic EOS below and indicate the revisions we will make.

read point-by-point responses
  1. Referee: [Abstract] Abstract (paragraph on calculations of moment of inertia and tidal deformability): the central claim that radii of 12–13 km are compatible with GW170817 and thereby identify suitable EOS rests on the assumption that the employed microscopic EOS remain accurate when extrapolated to the densities (~2–5 ρ_sat) and β-equilibrium asymmetries realized in neutron stars. The manuscript compares the pressure-density relation only to heavy-ion data at lower densities and different isospin; no independent cross-check (e.g., maximum-mass consistency or other NS observables independent of the same models) is described that would validate the extrapolation step itself.

    Authors: We agree that the extrapolation of microscopic EOS to the densities and asymmetries of neutron stars requires careful justification. The models in this work are constructed from approaches constrained by nuclear saturation properties and heavy-ion collision data up to approximately 2 ρ_sat. Neutron-star radii are predominantly sensitive to the EOS in the 1–3 ρ_sat range, which overlaps with the laboratory-constrained regime; the GW170817 radius constraint therefore tests the models where they are most directly anchored by data. The reported calculations of tidal deformability and moment of inertia, together with the confirmed universal relations, provide internal consistency checks. To strengthen the manuscript in response to this comment, we will revise the abstract and relevant sections to explicitly note that the EOS compatible with the 12–13 km radius range are also consistent with the ~2 M_⊙ maximum-mass constraint from pulsar timing, thereby supplying an independent high-density cross-check. revision: yes

Circularity Check

0 steps flagged

No significant circularity; radii 12-13 km obtained by applying external GW170817 constraints to independent microscopic EOS

full rationale

The derivation applies external GW170817 tidal deformability and radius bounds to a collection of pre-existing microscopic nuclear and hybrid EOS. Computed NS radii and deformabilities are compared to the event data to identify compatible models in the 12-13 km range. No step reduces a reported result to a parameter fitted inside this paper or to a self-citation chain that itself depends on the GW170817 outcome. Self-citations to prior EOS work exist but supply independent nuclear-theory input rather than load-bearing justification for the final radius selection. The extrapolation assumption is a correctness concern, not a circularity defect.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on the accuracy of the chosen microscopic EOS when applied to neutron-star densities and on the validity of the universal relations used for moment of inertia and tidal deformability; these are domain assumptions rather than new entities or free parameters introduced in the paper.

axioms (2)
  • domain assumption Microscopic equations of state calibrated to heavy-ion data remain reliable when extrapolated to the densities and asymmetries inside neutron stars.
    Invoked when the authors compute NS properties and compare with GW170817 constraints.
  • domain assumption Universal relations between moment of inertia, tidal deformability, and compactness hold for the hybrid-star configurations considered.
    Stated as confirmed in the abstract.

pith-pipeline@v0.9.0 · 5673 in / 1361 out tokens · 35677 ms · 2026-05-25T01:22:44.417205+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

75 extracted references · 75 canonical work pages · 3 internal anchors

  1. [1]

    J. M. Lattimer and M. Prakash, Neutron star observations: Prognosis for equation of state constraints, Phys. Rep. 442 (2007) 109

  2. [2]

    J. M. Lattimer, The nuclear equation of state and neutron star masses, Ann. Rev. Nucl. Sci. 62 (2012) 485

  3. [3]

    Özel and P

    F. Özel and P. Freire, Masses, Radii, and the Equation of State of Neutron Stars, Ann. Rev. Astron. Astrophys. 54 (2016) 401

  4. [4]

    Guillot, M

    S. Guillot, M. Servillat, N. A. Webb and R. E. Rutledge, Measurement of the radius of neutron stars with high signal-to-noise quiescent low-mass x-ray binaries in globular clusters, Astrophys. J. 772 (2013) 7

  5. [5]

    J. M. Lattimer and A. W. Steiner, Neutron Star Masses and Radii from Quiescent Low-Mass X-ray Binaries, Astrophys. J. 784 (2014) 123

  6. [6]

    J. M. Lattimer and M. Prakash, The equation of state of hot, dense matter and neutron stars, Phys. Rep. 621 (2016) 127

  7. [7]

    J. M. Lattimer and B. F. Schutz, Constraining the Equation of State with Moment of Inertia Measurements, Astrophys. J. 629 (2005) 979

  8. [8]

    Abbott et al., GW170817: Observation of Gravitational Waves from a Binary Neutron Star Inspiral, Phys

    V IRGO , LIGO S CIENTIFIC collaboration, B. Abbott et al., GW170817: Observation of Gravitational Waves from a Binary Neutron Star Inspiral, Phys. Rev. Lett. 119 (2017) 161101. 7 Constraints from the GW170817 merger event G. F. Burgio

  9. [9]

    J. B. Hartle, Slowly rotating relativistic stars. 1. Equations of structure, Astrophys. J. 150 (1967) 1005

  10. [10]

    E. E. Flanagan and T. Hinderer, Constraining neutron star tidal Love numbers with gravitational wave detectors, Phys. Rev. D 77 (2008) 021502

  11. [11]

    Radice, A

    D. Radice, A. Perego, F. Zappa and S. Bernuzzi, GW170817: Joint Constraint on the Neutron Star Equation of State from Multimessenger Observations, Astrophys. J. 852 (2018) L29

  12. [12]

    Yagi and N

    K. Yagi and N. Yunes, I-Love-Q Relations in Neutron Stars and their Applications to Astrophysics, Gravitational Waves and Fundamental Physics, Phys. Rev. D 88 (2013) 023009

  13. [13]

    Yagi and N

    K. Yagi and N. Yunes, Approximate Universal Relations for Neutron Stars and Quark Stars, Phys. Rept. 681 (2017) 1

  14. [14]

    G. F. Burgio and A. F. Fantina, Nuclear Equation of state for Compact Stars and Supernovae, ArXiv e-prints (2018) [ 1804.03020]

  15. [15]

    J. P. Jeukenne, A. Lejeune and C. Mahaux, Many-body theory of nuclear matter, Phys. Rep. 25 (1976) 83

  16. [16]

    Baldo, Nuclear Methods And The Nuclear Equation Of State, International Review of Nuclear Physics (World Scientific, Singapore)8 (1999)

    M. Baldo, Nuclear Methods And The Nuclear Equation Of State, International Review of Nuclear Physics (World Scientific, Singapore)8 (1999)

  17. [17]

    Z. H. Li and H. J. Schulze, Neutron star structure with modern nucleonic three-body forces, Phys. Rev. C 78 (2008) 028801

  18. [18]

    R. B. Wiringa, V . G. J. Stoks and R. Schiavilla,An Accurate nucleon-nucleon potential with charge independence breaking, Phys. Rev. C 51 (1995) 38

  19. [19]

    Machleidt, K

    R. Machleidt, K. Holinde and C. Elster, The Bonn Meson Exchange Model for the Nucleon Nucleon Interaction, Phys. Rept. 149 (1987) 1

  20. [20]

    Machleidt, The Meson theory of nuclear forces and nuclear structure, Adv

    R. Machleidt, The Meson theory of nuclear forces and nuclear structure, Adv. Nucl. Phys. 19 (1989) 189

  21. [21]

    M. M. Nagels, T. A. Rijken and J. J. de Swart, A Low-Energy Nucleon-Nucleon Potential from Regge Pole Theory, Phys. Rev. D 17 (1978) 768

  22. [22]

    V . G. J. Stoks, R. A. M. Klomp, C. P. F. Terheggen and J. J. de Swart,Construction of high quality N N potential models, Phys. Rev. C 49 (1994) 2950

  23. [23]

    Grangé, A

    P. Grangé, A. Lejeune, M. Martzolff and J.-F. Mathiot, Consistent three-nucleon forces in the nuclear many-body problem, Phys. Rev. C 40 (1989) 1040

  24. [24]

    Baldo, I

    M. Baldo, I. Bombaci and G. F. Burgio, Microscopic nuclear equation of state with three-body forces and neutron star structure, Astron. Astrophys. 328 (1997) 274

  25. [25]

    Z. H. Li, U. Lombardo, H.-J. Schulze and W. Zuo, Consistent nucleon-nucleon potentials and three-body forces, Phys. Rev. C 77 (2008) 034316

  26. [26]

    Gross-Boelting, C

    T. Gross-Boelting, C. Fuchs and A. Faessler, Covariant representations of the relativistic Brueckner T-matrix and the nuclear matter problem, Nucl. Phys. A 648 (1999) 105

  27. [27]

    Akmal, V

    A. Akmal, V . R. Pandharipande and D. G. Ravenhall,Equation of state of nucleon matter and neutron star structure, Phys. Rev. C 58 (1998) 1804

  28. [28]

    J. M. Lattimer and F. D. Swesty, A Generalized equation of state for hot, dense matter, Nucl. Phys. A 535 (1991) 331. 8 Constraints from the GW170817 merger event G. F. Burgio

  29. [29]

    A. W. Steiner, M. Hempel and T. Fischer, Core-collapse supernova equations of state based on neutron star observations, Astrophys. J. 774 (2013) 17

  30. [30]

    Chodos, R

    A. Chodos, R. L. Jaffe, K. Johnson, C. B. Thorn and V . F. Weisskopf,A New Extended Model of Hadrons, Phys. Rev. D 9 (1974) 3471

  31. [31]

    Buballa, NJL model analysis of quark matter at large density, Phys

    M. Buballa, NJL model analysis of quark matter at large density, Phys. Rept. 407 (2005) 205

  32. [32]

    Klähn and T

    T. Klähn and T. Fischer, Vector interaction enhanced bag model for astrophysical applications, Astrophys. J. 810 (2015) 134

  33. [33]

    C. D. Roberts and A. G. Williams, Dyson-Schwinger equations and their application to hadronic physics, Prog. Part. Nucl. Phys.33 (1994) 477

  34. [34]

    Alkofer and L

    R. Alkofer and L. von Smekal, The Infrared behavior of QCD Green’s functions: Confinement dynamical symmetry breaking, and hadrons as relativistic bound states, Phys. Rept. 353 (2001) 281

  35. [35]

    H. Chen, M. Baldo, G. F. Burgio and H.-J. Schulze, Hybrid stars with the Dyson-Schwinger quark model, Phys. Rev. D 84 (2011) 105023

  36. [36]

    J. B. Wei, H. Chen and H. J. Schulze, Two-flavor hybrid stars with the Dyson-Schwinger quark model, Chin. Phys. C 41 (2017) 115101

  37. [37]

    P. B. Demorest, T. Pennucci, S. M. Ransom, M. S. Roberts and J. W. Hessels, A two-solar-mass neutron star measured using shapiro delay, Nature 467 (2010) 1081

  38. [38]

    Fonseca et al., The NANOGrav Nine-year Data Set: Mass and Geometric Measurements of Binary Millisecond Pulsars, Astrophys

    E. Fonseca et al., The NANOGrav Nine-year Data Set: Mass and Geometric Measurements of Binary Millisecond Pulsars, Astrophys. J. 832 (2016) 167

  39. [39]

    Antoniadis et al., A Massive Pulsar in a Compact Relativistic Binary, Science 340 (2013) 6131

    J. Antoniadis et al., A Massive Pulsar in a Compact Relativistic Binary, Science 340 (2013) 6131

  40. [40]

    H. J. Schulze, A. Polls, A. Ramos and I. Vidana, Maximum mass of neutron stars, Phys. Rev. C 73 (2006) 058801

  41. [41]

    T. A. Rijken and H.-J. Schulze, Hyperon-hyperon interactions with the Nijmegen ESC08 model, Eur. Phys. J. A 52 (2016) 21

  42. [42]

    Schulze and T

    H.-J. Schulze and T. Rijken, Maximum mass of hyperon stars with the Nijmegen ESC08 model, Phys. Rev. C 84 (2011) 035801

  43. [43]

    Drago, A

    A. Drago, A. Lavagno, G. Pagliara and D. Pigato, The scenario of two families of compact stars, Eur. Phys. J. A 52 (2016) 40

  44. [44]

    Drago and G

    A. Drago and G. Pagliara, Merger of two neutron stars: predictions from the two-families scenario, Astrophys. J. 852 (2018) L32

  45. [45]

    G. F. Burgio, A. Drago, G. Pagliara, H. J. Schulze and J. B. Wei, Are Small Radii of Compact Stars Ruled out by GW170817/AT2017gfo?, Astrophys. J. 860 (2018) 139

  46. [46]

    Paschalidis, K

    V . Paschalidis, K. Yagi, D. Alvarez-Castillo, D. B. Blaschke and A. Sedrakian,Implications from GW170817 and I-Love-Q relations for relativistic hybrid stars, Phys. Rev. D 97 (2018) 084038

  47. [47]

    Danielewicz, R

    P. Danielewicz, R. Lacey and W. G. Lynch, Determination of the Equation of State of Dense Matter, Science 298 (2002) 1592

  48. [48]

    J. L. Ritman, N. Herrmann, D. Best, J. P. Alard, V . Amouroux, N. Bastid et al.,On the transverse momentum distribution of strange hadrons produced in relativistic heavy ion collisions, Zeitschrift fur Physik A Hadrons and Nuclei 352 (1995) 355. 9 Constraints from the GW170817 merger event G. F. Burgio

  49. [49]

    Mi ´skowiec, W

    D. Mi ´skowiec, W. Ahner, R. Barth, M. Cie´slak, M. De ¸bowski, E. Grosse et al.,Observation of enhanced subthreshold K+ production in central collisions between heavy nuclei, Phys. Rev. Lett. 72 (1994) 3650

  50. [50]

    G. Colò, N. van Giai, J. Meyer, K. Bennaceur and P. Bonche, Microscopic determination of the nuclear incompressibility within the nonrelativistic framework, Phys. Rev. C 70 (2004) 024307

  51. [51]

    V IRGO , LIGO S CIENTIFIC collaboration, B. P. Abbott et al., GW170817: Measurements of neutron star radii and equation of state, Phys. Rev. Lett. 121 (2018) 161101

  52. [52]

    C. Y . Tsang, M. B. Tsang, P. Danielewicz, W. G. Lynch and F. J. Fattoyev,Constraining neutron-star equation of state using heavy-ion collisions, ArXiv e-prints (2018) [ 1807.06571]

  53. [53]

    Shibata, S

    M. Shibata, S. Fujibayashi, K. Hotokezaka, K. Kiuchi, K. Kyutoku, Y . Sekiguchi et al., Modeling GW170817 based on numerical relativity and its implications, Phys. Rev. D 96 (2017) 123012

  54. [54]

    Margalit and B

    B. Margalit and B. D. Metzger, Constraining the Maximum Mass of Neutron Stars From Multi-Messenger Observations of GW170817, Astrophys. J. 850 (2017) L19

  55. [55]

    Rezzolla, E

    L. Rezzolla, E. R. Most and L. R. Weih, Using gravitational-wave observations and quasi-universal relations to constrain the maximum mass of neutron stars, Astrophys. J. 852 (2018) L25

  56. [56]

    Annala, T

    E. Annala, T. Gorda, A. Kurkela and A. Vuorinen, Gravitational-wave constraints on the neutron-star-matter Equation of State, Phys. Rev. Lett. 120 (2018) 172703

  57. [57]

    E. R. Most, L. R. Weih, L. Rezzolla and J. Schaffner-Bielich, New constraints on radii and tidal deformabilities of neutron stars from GW170817, Phys. Rev. Lett. 120 (2018) 261103

  58. [58]

    Lim and J

    Y . Lim and J. W. Holt,Neutron star tidal deformabilities constrained by nuclear theory and experiment, Phys. Rev. Lett. 121 (2018) 062701

  59. [59]

    Raithel, F

    C. Raithel, F. Özel and D. Psaltis, Tidal deformability from GW170817 as a direct probe of the neutron star radius, Astrophys. J. 857 (2018) L23

  60. [60]

    Bauswein, O

    A. Bauswein, O. Just, H.-T. Janka and N. Stergioulas, Neutron-star radius constraints from GW170817 and future detections, Astrophys. J. 850 (2017) L34

  61. [61]

    Pian et al., Spectroscopic identification of r-process nucleosynthesis in a double neutron star merger, Nature 551 (2017) 67

    E. Pian et al., Spectroscopic identification of r-process nucleosynthesis in a double neutron star merger, Nature 551 (2017) 67

  62. [62]

    D. A. Coulter et al., Swope Supernova Survey 2017a (SSS17a), the Optical Counterpart to a Gravitational Wave Source, Science 358 (2017) 1556

  63. [63]

    P. S. Cowperthwaite et al., The Electromagnetic Counterpart of the Binary Neutron Star Merger LIGO/Virgo GW170817. II. UV , Optical, and Near-infrared Light Curves and Comparison to Kilonova Models, Astrophys. J. 848 (2017) L17

  64. [64]

    Nicholl et al., The Electromagnetic Counterpart of the Binary Neutron Star Merger LIGO/VIRGO GW170817

    M. Nicholl et al., The Electromagnetic Counterpart of the Binary Neutron Star Merger LIGO/VIRGO GW170817. III. Optical and UV Spectra of a Blue Kilonova From Fast Polar Ejecta, Astrophys. J. 848 (2017) L18

  65. [65]

    K. D. Alexander et al., The Electromagnetic Counterpart of the Binary Neutron Star Merger LIGO/VIRGO GW170817. VI. Radio Constraints on a Relativistic Jet and Predictions for Late-Time Emission from the Kilonova Ejecta, Astrophys. J. 848 (2017) L21

  66. [66]

    J. M. Lattimer and M. Prakash, Neutron star structure and the equation of state, Astrophys. J. 550 (2001) 426. 10 Constraints from the GW170817 merger event G. F. Burgio

  67. [67]

    A. W. Steiner, J. M. Lattimer and E. F. Brown, The equation of state from observed masses and radii of neutron stars, Astrophys. J. 722 (2010) 33

  68. [68]

    A. W. Steiner, J. M. Lattimer and E. F. Brown, The neutron star mass-radius relation and the equation of state of dense matter, Astrophys. J. Lett. 765 (2013) L5

  69. [69]

    Wiktorowicz, A

    G. Wiktorowicz, A. Drago, G. Pagliara and S. B. Popov, Strange quark stars in binaries: formation rates, mergers and explosive phenomena, Astrophys. J. 846 (2017) 163

  70. [70]

    Hinderer, Tidal Love numbers of neutron stars, Astrophys

    T. Hinderer, Tidal Love numbers of neutron stars, Astrophys. J. 677 (2008) 1216

  71. [71]

    tidal love numbers of neutron stars

    T. Hinderer, Erratum: "tidal love numbers of neutron stars" (2008, apj, 677, 1216), Astrophys. J. 697 (2009) 964

  72. [72]

    Hinderer, B

    T. Hinderer, B. D. Lackey, R. N. Lang and J. S. Read, Tidal deformability of neutron stars with realistic equations of state and their gravitational wave signatures in binary inspiral, Phys. Rev. D 81 (2010) 123016

  73. [73]

    Worley, P

    A. Worley, P. G. Krastev and B.-A. Li, Nuclear constraints on the momenta of inertia of neutron stars, Astrophys. J. 685 (2008) 390

  74. [74]

    J.-B. Wei, A. Figura, G. F. Burgio, H. Chen and H.-J. Schulze, Neutron star universal relations with microscopic equations of state, ArXiv e-prints (2018) [ 1809.04315]

  75. [75]

    Breu and L

    C. Breu and L. Rezzolla, Maximum mass, moment of inertia and compactness of relativistic stars, Mon. Not. Roy. Astron. Soc. 459 (2016) 646. 11