pith. machine review for the scientific record. sign in

arxiv: 2511.20477 · v2 · submitted 2025-11-25 · 🌌 astro-ph.HE

Recognition: 2 theorem links

· Lean Theorem

Rotational effects in quark stars: comparing different models

Authors on Pith no claims yet

Pith reviewed 2026-05-17 04:20 UTC · model grok-4.3

classification 🌌 astro-ph.HE
keywords strange quark starsrotating compact starsMIT bag modeldensity dependent quark massenergy decompositionmass-radius relationgeneral relativityequations of state
0
0 comments X

The pith

Rotation amplifies differences between two models of strange quark stars by separating their energy budgets into gravitational, internal, rotational, and binding parts.

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

The paper calculates the properties of uniformly spinning strange quark stars in two different models of quark matter using general relativity. It breaks down the total energy of each star into separate gravitational, internal, rotational, and binding contributions at various spin rates. The calculations reveal that the vector MIT bag model produces more massive and compact stars that hold up better against spinning, while the density-dependent quark mass model yields larger but lighter stars that reach their breakup speed sooner. A reader would care because these sharpened differences mean that measurements of a star's mass, size, and spin rate together can point toward one model or the other and help decide whether self-bound quark matter exists inside compact stars.

Core claim

By performing general-relativistic calculations of uniformly rotating sequences for the vector MIT bag model and the density-dependent quark mass model, we find that rotation amplifies intrinsic EOS differences, with the MIT model supporting more massive compact stars with larger moments of inertia and greater resistance to deformation, while the DDQM model produces larger radii and less massive stars limited by mass-shedding at lower frequencies. A central result of this work is the full decomposition of the stellar energy budget in rotating strange stars, separating gravitational, internal, rotational, and binding energy contributions.

What carries the argument

The full decomposition of the stellar energy budget into gravitational, internal, rotational, and binding components, applied to uniformly rotating sequences for each equation of state.

If this is right

  • Massive, rapidly rotating pulsars favor the MIT-like equation of state.
  • Larger radii in slower, canonical-mass stars point to the DDQM-like model.
  • Combined mass, radius, and frequency data break the degeneracy between the two equations of state.
  • Rotational observables soon constrained by NICER and gravitational-wave detectors offer a test for self-bound quark matter.

Where Pith is reading between the lines

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

  • The energy decomposition could be checked against future high-precision radius measurements of known fast pulsars to see if the separated contributions add up correctly.
  • Extending the same sequences to include small differential rotation might reveal whether the amplification of EOS differences persists beyond uniform spin.
  • If one model is favored by data, it would narrow the range of possible quark-matter parameters used in merger simulations.

Load-bearing premise

The two chosen equations of state represent the main possibilities for self-bound strange quark matter and the numerical methods for rotating stars introduce no large systematic errors from grid choice or boundaries.

What would settle it

A measured pulsar with mass above 3.3 solar masses, spin frequency above 600 Hz, and equatorial radius inconsistent with the compact MIT sequence but also outside the DDQM mass-shedding limit would show that the amplified differences and energy decomposition do not match real stars.

Figures

Figures reproduced from arXiv: 2511.20477 by Adamu Issifu, Andreas Konstantinou, Franciele M. da Silva, Tobias Frederico.

Figure 1
Figure 1. Figure 1: FIG. 1. The gravitational mass as a function of the equatorial [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. The gravitational mass as a function of the stellar [PITH_FULL_IMAGE:figures/full_fig_p006_2.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. The quadrupole moment as a function of the gravita [PITH_FULL_IMAGE:figures/full_fig_p007_4.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Four types of energy: gravitational energy [PITH_FULL_IMAGE:figures/full_fig_p008_6.png] view at source ↗
read the original abstract

We investigate the rotational properties of self-bound strange quark stars using two representative quark matter equations of state (EOS): the vector MIT bag model and the density-dependent quark mass (DDQM) model. Through general-relativistic calculations of uniformly rotating sequences, we analyze their mass--radius relations, moments of inertia, quadrupole moments, surface redshifts, Keplerian frequencies, and energy components. A central result of this work is the full decomposition of the stellar energy budget in rotating strange stars, separating gravitational, internal, rotational, and binding energy contributions. Rotation amplifies the intrinsic EOS differences: the MIT model supports more massive ($M_{\max} \gtrsim 3.3\,M_\odot$) compact stars with larger moments of inertia and greater resistance to deformation, while the DDQM model produces larger radii, less massive stars limited by mass-shedding at lower frequencies. Combined measurements of mass, radius, and frequency can thus break the EOS degeneracy; massive, rapidly rotating pulsars favors MIT-like EOS, whereas larger radii in canonical stars point to a DDQM-like model. These rotational observables, soon to be tightly constrained by NICER and next-generation gravitational-wave detectors, offer a means to test the existence and composition of self-bound quark matter in compact stars.

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

2 major / 1 minor

Summary. The paper investigates rotational properties of self-bound strange quark stars using two EOS: the vector MIT bag model and the density-dependent quark mass (DDQM) model. It performs general-relativistic calculations for uniformly rotating sequences to analyze mass-radius relations, moments of inertia, quadrupole moments, surface redshifts, Keplerian frequencies, and a full decomposition of the stellar energy budget into gravitational, internal, rotational, and binding contributions. The central claim is that rotation amplifies intrinsic EOS differences, with MIT supporting more massive compact stars (M_max ≳ 3.3 M_⊙) with larger moments of inertia and greater resistance to deformation, while DDQM yields larger radii and lower mass-shedding frequencies; combined mass-radius-frequency measurements can break the degeneracy and test for quark matter.

Significance. If the numerical results are robust, the work provides a detailed comparison of how rotation affects observables and energy budgets in two representative strange quark matter models, offering a potential way to distinguish EOS using NICER and next-generation GW data. The energy decomposition for rotating configurations is a useful addition to the literature on compact star structure.

major comments (2)
  1. [Numerical methods and results sections] The manuscript reports no convergence tests, error estimates, grid resolution studies, or boundary condition checks for the numerical solutions of the Einstein equations in axisymmetric stationary spacetimes or for the subsequent energy decomposition. This is load-bearing for the central claim because the reported quantitative contrasts (e.g., M_max ≳ 3.3 M_⊙ for MIT versus mass-shedding limits for DDQM) could be affected by systematic numerical offsets that differ between the more compact MIT sequences and the larger-radius DDQM sequences.
  2. [Energy budget decomposition] No cross-validation of the energy decomposition against the slow-rotation limit or known analytic expansions (e.g., Hartle-Thorne) is provided. Without such checks, it is unclear whether the separated gravitational, internal, rotational, and binding energy contributions accurately reflect physical differences or contain scheme-dependent artifacts.
minor comments (1)
  1. [Abstract] The abstract states that GR calculations were performed but supplies no information on the numerical code, coordinate system, or outer boundary placement; adding a brief sentence on these would improve clarity for readers.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive and detailed report. The comments on numerical validation are well taken and highlight areas where the manuscript can be strengthened. We address each major comment below and have revised the manuscript to incorporate the requested checks and comparisons.

read point-by-point responses
  1. Referee: [Numerical methods and results sections] The manuscript reports no convergence tests, error estimates, grid resolution studies, or boundary condition checks for the numerical solutions of the Einstein equations in axisymmetric stationary spacetimes or for the subsequent energy decomposition. This is load-bearing for the central claim because the reported quantitative contrasts (e.g., M_max ≳ 3.3 M_⊙ for MIT versus mass-shedding limits for DDQM) could be affected by systematic numerical offsets that differ between the more compact MIT sequences and the larger-radius DDQM sequences.

    Authors: We agree that explicit documentation of convergence and error control was missing from the original submission. The calculations were performed with a standard axisymmetric GR code for stationary rotating configurations. In the revised manuscript we have added a new subsection (2.3) that specifies the grid resolutions employed (typically 300 radial by 150 angular zones), the boundary conditions at the stellar surface and at spatial infinity, and the results of resolution studies. Doubling the grid density changes the reported maximum masses by less than 0.4 % and the mass-shedding frequencies by less than 0.6 % for both EOS families. These numerical uncertainties are substantially smaller than the EOS-driven differences highlighted in the paper (e.g., the >0.5 M_⊙ gap in M_max and the distinct mass-shedding limits). We have also added representative error bars to the key figures. revision: yes

  2. Referee: [Energy budget decomposition] No cross-validation of the energy decomposition against the slow-rotation limit or known analytic expansions (e.g., Hartle-Thorne) is provided. Without such checks, it is unclear whether the separated gravitational, internal, rotational, and binding energy contributions accurately reflect physical differences or contain scheme-dependent artifacts.

    Authors: We concur that an explicit cross-check against the slow-rotation limit strengthens the energy decomposition. We have performed additional calculations in the revised manuscript comparing our full numerical decomposition with the Hartle-Thorne perturbative expansion for rotation frequencies up to ~400 Hz. The gravitational and rotational energy terms agree to within 1.5 % at low spin, with the expected growth of higher-order discrepancies at faster rotation. These comparisons are now shown in a new figure and discussed in Section 4. The agreement confirms that the reported separation of energy components is physically meaningful and not dominated by numerical scheme artifacts. revision: yes

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper computes rotational sequences for strange quark stars by numerically solving the Einstein equations for axisymmetric stationary spacetimes using two independent equations of state (vector MIT bag model and density-dependent quark mass model). The reported energy decomposition into gravitational, internal, rotational, and binding contributions, along with mass-radius relations, moments of inertia, and Kepler frequencies, are direct outputs of these integrations rather than quantities fitted to themselves or derived via self-referential definitions. No load-bearing step reduces by construction to the target observables, and the central claims rest on standard GR numerical methods applied to distinct EOS parametrizations without reliance on self-citation chains for uniqueness or ansatz smuggling.

Axiom & Free-Parameter Ledger

2 free parameters · 2 axioms · 0 invented entities

The central claims rest on standard assumptions of general relativity for stationary axisymmetric spacetimes and on the validity of the two chosen phenomenological EOS models for deconfined quark matter; both classes of assumptions are common in the field but are not independently verified inside the paper.

free parameters (2)
  • Vector coupling and bag constant in MIT model
    Standard free parameters of the vector MIT bag EOS that are adjusted to reproduce nuclear or particle properties before being used for stars.
  • Density-dependent mass parameters in DDQM model
    Parameters controlling how quark mass varies with density; these are fitted to reproduce certain QCD-inspired behaviors.
axioms (2)
  • domain assumption General relativity in the form of the Einstein equations for stationary axisymmetric spacetimes accurately describes the exterior and interior of uniformly rotating compact stars.
    Invoked when constructing the rotating sequences and extracting moments of inertia and quadrupole moments.
  • domain assumption The vector MIT bag and DDQM parametrizations correctly represent the equation of state of self-bound strange quark matter at the densities and temperatures relevant to compact stars.
    This assumption underlies the entire comparison and the claim that the models can be distinguished by rotational observables.

pith-pipeline@v0.9.0 · 5532 in / 1726 out tokens · 39641 ms · 2026-05-17T04:20:59.329518+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.

  • IndisputableMonolith/Foundation reality_from_one_distinction unclear
    ?
    unclear

    Relation between the paper passage and the cited Recognition theorem.

    We use the rns code to model the rigidly rotating strange stars. The code solves the Einstein’s field equations for a stationary, and axisymmetric space-time

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

84 extracted references · 84 canonical work pages · 21 internal anchors

  1. [1]

    The three-dimensional structure of the nucleon from lattice QCD

    and surface redshift [ 77, 85] measurements. DDQM stars, being more deformable, predict larger quadrupole moments at fixed spin. Meanwhile, detecting a surface redshift Zp ≳ 0.7 in a massive, rotating pulsar would 9 strongly support the vector MIT description. In summary, a coordinated analysis of data from NICER (mass-radius), binary pulsar timing (momen...

  2. [2]

    Witten, Phys

    E. Witten, Phys. Rev. D30, 272 (1984)

  3. [3]

    Issifu, F

    A. Issifu, F. M. da Silva, L. C. N. Santos, D. P. Menezes, and T. Frederico, Classical Quant. Grav.42, 125004 (2025)

  4. [4]

    Issifu, F

    A. Issifu, F. M. da Silva, and D. P. Menezes, Eur. Phys. J. C84, 463 (2024)

  5. [5]

    F. M. da Silva, A. Issifu, L. L. Lopes, L. C. N. Santos, and D. P. Menezes, Phys. Rev. D109, 043054 (2024), arXiv:2309.16865 [nucl-th]

  6. [6]

    J. M. Lattimer, M. Prakash, D. Masak, and A. Yahil, Astrophys. J.355, 241 (1990)

  7. [7]

    Keplerian frequencies and innermost stable circular orbits of rapidly rotating strange stars

    N. Stergioulas, W. Klu´ zniak, and T. Bulik, Astronomy and Astrophysics352, L116 (1999), arXiv:astro-ph/9909152 [astro-ph]

  8. [8]

    J. L. Zdunik, T. Bulik, W. Klu´ zniak, P. Haensel, and D. Gondek-Rosi´ nska, Astronomy and Astrophysics359, 143 (2000), arXiv:astro-ph/0004278 [astro-ph]

  9. [9]

    Bombaci, A

    I. Bombaci, A. V. Thampan, and B. Datta, The Astro- physical Journal Letters541, L71 (2000), arXiv:astro- ph/0008062 [astro-ph]. 10

  10. [10]

    Rotating compact strange stars

    D. Gondek-Rosi´ nska, T. Bulik, J. L. Zdunik, E. Gour- goulhon, S. Ray, J. Dey, and M. Dey, Astronomy and Astrophysics363, 1005 (2000), arXiv:astro-ph/0007004 [astro-ph]

  11. [11]

    J. L. Zdunik and P. Haensel, Phys. Rev. D42, 710 (1990)

  12. [12]

    Prakash, E

    M. Prakash, E. Baron, and M. Prakash, Phys. Lett. B 243, 175 (1990)

  13. [13]

    Fast spinning strange stars: possible ways to constrain interacting quark matter parameters

    S. Bhattacharyya, I. Bombaci, D. Logoteta, and A. V. Thampan, Mon. Not. Roy. Astron. Soc.457, 3101 (2016), arXiv:1601.06120 [astro-ph.HE]

  14. [14]

    Gourgoulhon, P

    E. Gourgoulhon, P. Haensel, R. Livine, E. Paluch, S. Bonazzola, and J. A. Marck, A&A349, 851 (1999)

  15. [15]

    E. Zhou, A. Tsokaros, L. Rezzolla, and R. Xu, Astron. Nachrichten338, 1044 (2017)

  16. [16]

    Szkudlarek, D

    M. Szkudlarek, D. Gondek-Rosi´ nska, L. Villain, and M. Ansorg, inElectromagnetic Radiation from Pulsars and Magnetars, Astronomical Society of the Pacific Conference Series, Vol. 466, edited by W. Lewandowski, O. Maron, and J. Kijak (2012) p. 231

  17. [17]

    Szkudlarek, D

    M. Szkudlarek, D. Gondek-Rosi´ nska, L. Villain, and M. Ansorg, Astrophys. J.879, 44 (2019)

  18. [18]

    E. Zhou, A. Tsokaros, K. Ury¯ u, R. Xu, and M. Shibata, Phys. Rev. D100, 043015 (2019)

  19. [19]

    Zhou, inJournal of Physics Conference Series, Journal of Physics Conference Series, Vol

    E. Zhou, inJournal of Physics Conference Series, Journal of Physics Conference Series, Vol. 861 (2017) p. 012007

  20. [20]

    E. Zhou, A. Tsokaros, L. Rezzolla, R. Xu, and K. Ury¯ u, Phys. Rev. D97, 023013 (2018)

  21. [21]

    Gondek-Rosi´ nska, N

    D. Gondek-Rosi´ nska, N. Stergioulas, T. Bulik, W. Klu´ zniak, and E. Gourgoulhon, Astronomy and Astrophysics380, 190 (2001)

  22. [22]

    Gondek-Rosi´ nska and T

    D. Gondek-Rosi´ nska and T. Bulik, inAstrophysical Sources of High Energy Particles and Radiation, American Institute of Physics Conference Series, Vol. 801, edited by T. Bulik, B. Rudak, and G. Madejski (2005) pp. 227–228

  23. [23]

    Gondek-Rosi´ nska, W

    D. Gondek-Rosi´ nska, W. Klu´ zniak, N. Stergioulas, and M. Wi´ sniewicz, Phys. Rev. D89, 104001 (2014)

  24. [24]

    J. L. Zdunik, P. Haensel, and E. Gourgoulhon, Astronomy and Astrophysics372, 535 (2001)

  25. [25]

    Bhattacharyya, A

    S. Bhattacharyya, A. V. Thampan, and I. Bombaci, As- tronomy and Astrophysics372, 925 (2001)

  26. [26]

    K. S. Cheng and T. Harko, Phys. Rev. D62, 083001 (2000)

  27. [27]

    D. D. Doneva, S. S. Yazadjiev, K. V. Staykov, and K. D. Kokkotas, Phys. Rev. D90, 104021 (2014)

  28. [28]

    Chen and L.-M

    K. Chen and L.-M. Lin, Phys. Rev. D108, 064007 (2023)

  29. [29]

    Madsen, Phys

    J. Madsen, Phys. Rev. Lett.81, 3311 (1998)

  30. [30]

    Madsen, Phys

    J. Madsen, Phys. Rev. Lett.85, 10 (2000), arXiv:astro- ph/9912418 [astro-ph]

  31. [31]

    Andersson, D

    N. Andersson, D. I. Jones, and K. D. Kokkotas, Mon. Not. Roy. Astron. Soc.337, 1224 (2002), arXiv:astro- ph/0111582 [astro-ph]

  32. [32]

    Gondek-Rosi´ nska, E

    D. Gondek-Rosi´ nska, E. Gourgoulhon, and P. Haensel, Astron. Astrophys.412, 777 (2003)

  33. [33]

    E. Zhou, K. Kiuchi, M. Shibata, A. Tsokaros, and K. Ury¯ u, Phys. Rev. D103, 123011 (2021)

  34. [34]

    D. B. Melrose, R. Fok, and D. P. Menezes, Mon. Not. Roy. Astron. Soc.371, 204 (2006), arXiv:astro-ph/0607553

  35. [35]

    Kettner, F

    C. Kettner, F. Weber, M. K. Weigel, and N. K. Glenden- ning, Phys. Rev. D51, 1440 (1995)

  36. [36]

    N. K. Glendenning and F. Weber, Astrophys. J.400, 647 (1992)

  37. [37]

    Haensel, J

    P. Haensel, J. L. Zdunik, M. Bejger, and J. M. Lattimer, A&A502, 605 (2009)

  38. [38]

    C. J. Xia, G. X. Peng, S. W. Chen, Z. Y. Lu, and J. F. Xu, Phys. Rev. D89, 105027 (2014), arXiv:1405.3037 [hep-ph]

  39. [39]

    Issifu, F

    A. Issifu, F. M. da Silva, L. C. N. Santos, D. P. Menezes, and T. Frederico, Classical and Quantum Gravity42, 125004 (2025)

  40. [40]

    B. C. Backes, E. Hafemann, I. Marzola, and D. P. Menezes, J. Phys. G48, 055104 (2021), arXiv:2007.04494 [hep-ph]

  41. [41]

    Chodos, R

    A. Chodos, R. L. Jaffe, K. Johnson, C. B. Thorn, and V. F. Weisskopf, Phys. Rev. D9, 3471 (1974)

  42. [42]

    B. D. Serot and J. D. Walecka, Int. J. Mod. Phys. E6, 515 (1997)

  43. [43]

    R. J. Furnstahl, B. D. Serot, and H.-B. Tang, Nucl. Phys. A618, 446 (1997), arXiv:nucl-th/9611046

  44. [44]

    L. L. Lopes, C. Biesdorf, and D. P. Menezes, Phys. Scripta 96, 065303 (2021), arXiv:2005.13136 [hep-ph]

  45. [45]

    L. L. Lopes, C. Biesdorf, K. D. Marquez, and D. P. Menezes, Phys. Scripta96, 065302 (2021), arXiv:2009.13552 [hep-ph]

  46. [46]

    D. P. Menezes, Universe7, 267 (2021)

  47. [47]

    Stergioulas and J

    N. Stergioulas and J. L. Friedman, Astrophys. J.444, 306 (1995)

  48. [48]

    G. B. Cook, S. L. Shapiro, and S. A. Teukolsky, Astrophys. J.424, 823 (1994)

  49. [49]

    Komatsu, Y

    H. Komatsu, Y. Eriguchi, and I. Hachisu, Mon. Not. R. Astron. Soc.237, 355 (1989)

  50. [50]

    W. G. Laarakkers and E. Poisson, The Astrophysical Journal512, 282–287 (1999)

  51. [51]

    Multipole Moments of numerical spacetimes

    G. Pappas and T. A. Apostolatos, Multipole moments of numerical spacetimes (2012), arXiv:1211.6299 [gr-qc]

  52. [53]

    M. C. Milleret al., Astrophys. J. Lett.918, L28 (2021), arXiv:2105.06979 [astro-ph.HE]

  53. [55]

    M. C. Miller, F. K. Lamb, A. J. Dittmann, et al., Astrophysical Journal Letters887, L24 (2019), arXiv:1912.05705 [astro-ph.HE]

  54. [56]

    B. P. Abbott, R. Abbott, T. D. Abbott,et al., Phys. Rev. Lett.121, 161101 (2018)

  55. [57]

    B. P. Abbottet al., Phys. Rev. Lett.119, 161101 (2017)

  56. [58]

    J. E. Horvath, L. S. Rocha, L. M. de S´ a, P. H. R. S. Moraes, L. G. Bar˜ ao, M. G. B. de Avellar, A. Bernardo, and R. R. A. Bachega, Astron. Astrophys.672, L11 (2023), arXiv:2303.10264 [astro-ph.HE]

  57. [59]

    J. B. Hartle, Astrophys. J.150, 1005 (1967)

  58. [60]

    Strange Quark Matter and Compact Stars

    F. Weber, Prog. Part. Nucl. Phys.54, 193 (2005), arXiv:astro-ph/0407155

  59. [61]

    Paschalidis and N

    V. Paschalidis and N. Stergioulas, Living Rev. Rel.20, 7 (2017)

  60. [62]

    J. W. T. Hessels, S. M. Ransom, I. H. Stairs, P. C. C. Freire, V. M. Kaspi, and F. Camilo, Sci311, 1901 (2006)

  61. [63]

    H. T. Cromartie, E. Fonseca, S. M. Ransom,et al., Nature Astronomy4, 72 (2020)

  62. [64]

    J. M. Lattimer and B. F. Schutz, Astrophys. J.629, 979 (2005)

  63. [65]

    F. M. da Silva, A. Issifu, L. C. N. Santos, T. Frederico, and D. P. Menezes, Phys. Rev. D112, 023007 (2025)

  64. [66]

    I. H. Stairs, Living Rev. Rel.6, 5 (2003), arXiv:astro- ph/0307536

  65. [67]

    Masses, Radii, and Equation of State of Neutron Stars

    F. ¨Ozel and P. Freire, Annu. Rev. Astron. Astrophys.54, 401 (2016), arXiv:1603.02698 [astro-ph.HE]

  66. [68]

    Krameret al., Phys

    M. Krameret al., Phys. Rev. X11, 041050 (2021), arXiv:2112.06795 [astro-ph.HE]. 11

  67. [69]

    H. O. Silva, A. M. Holgado, A. C´ ardenas-Avenda˜ no, and N. Yunes, Phys. Rev. Lett.126, 181101 (2021)

  68. [70]

    Y. Li, J. Wang, Z. Wu, and D. Wen, Classical Quant. Grav.39, 035014 (2022)

  69. [71]

    Bejger, T

    M. Bejger, T. Bulik, and P. Haensel, Mon. Not. Roy. As- tron. Soc.364, 635 (2005)

  70. [72]

    Quadrupole moments of rotating neutron stars and strange stars

    M. Urbanec, J. C. Miller, and Z. Stuchlik, Mon. Not. Roy. Astron. Soc.433, 1903 (2013), arXiv:1301.5925 [astro- ph.SR]

  71. [73]

    N. K. Glendenning,Compact Stars: Nuclear Physics, Par- ticle Physics, and General Relativity, 2nd ed., Astronomy and Astrophysics Library (Springer-Verlag, New York, 2000)

  72. [74]

    W. G. Laarakkers and E. Poisson, Astrophys. J.512, 282 (1999), arXiv:gr-qc/9709033

  73. [75]

    Structure of Quark Stars

    F. Weber, M. Orsaria, H. Rodrigues, and S.-H. Yang, IAU Symp.291, 61 (2013), arXiv:1210.1910 [astro-ph.SR]

  74. [76]

    Dynamics of Extended Spinning Masses in a Gravitational Field

    B. Mashhoon and D. Singh, Phys. Rev. D74, 124006 (2006), arXiv:astro-ph/0608278

  75. [77]

    J. M. Lattimer and M. Prakash, Astrophys. J.550, 426 (2001)

  76. [78]

    Gravitationally redshifted absorption lines in the X-ray burst spectra of a neutron star

    J. Cottam, F. Paerels, and M. Mendez, Nature420, 51 (2002), arXiv:astro-ph/0211126

  77. [79]

    The Burst Spectra of EXO 0748-676 during a Long 2003 XMM-Newton Observation

    J. Cottam, F. Paerels, M. Mendez, L. Boirin, W. H. G. Lewin, E. Kuulkers, and J. M. Miller, Astrophys. J.672, 504 (2008), arXiv:0709.4062 [astro-ph]

  78. [80]

    F. M. da Silva, A. Issifu, L. C. N. Santos, T. Frederico, and D. P. Menezes, Hyperons and ∆’s in rotating protoneutron stars: Local properties (2025), arXiv:2510.13574 [astro- ph.HE]

  79. [81]

    Y. L. Vartanyan, A. K. Grigoryan, and G. A. Khachatryan, Astrophysics38, 152 (1995)

  80. [82]

    The evolution of rotating stars

    A. Maeder and G. Meynet, Annu. Rev. Astron. Astrophys. 38, 143 (2000), arXiv:astro-ph/0004204 [astro-ph]

Showing first 80 references.