pith. sign in

arxiv: 2604.04617 · v2 · submitted 2026-04-06 · 🌀 gr-qc · astro-ph.SR· hep-th

Preliminary study on the impact of stress-energy tensor compared to scalar field in Nonminimal Derivative model

Pith reviewed 2026-05-12 02:11 UTC · model grok-4.3

classification 🌀 gr-qc astro-ph.SRhep-th
keywords Nonminimal Derivative Couplingstress-energy tensorscalar fieldincompressible starcompactnessmass-radius relationmodified gravity
0
0 comments X

The pith

Coupling parameters in the NMDC-T model prove less sensitive than in NMDC-phi when modeling incompressible stars.

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

This paper compares two versions of the Nonminimal Derivative Coupling gravitational model: NMDC-T, which incorporates the trace of the stress-energy tensor, and NMDC-phi, which uses a real-valued scalar field. Both versions are inserted into the equations for an incompressible star to measure changes in compactness and the mass-radius relation. The central result is that variations in the coupling parameter produce smaller shifts in these stellar properties for NMDC-T than for NMDC-phi. A reader would care because the finding bears on how freely the coupling strength can be varied while still producing stable predictions for compact objects.

Core claim

We report the results of comparing the effect of using trace of stress-energy tensor versus real-valued scalar field in Nonminimal Derivative Coupling gravitation model, respectively denoted as NMDC-T and NMDC-phi. We employ the model into an incompressible star and see the effect of both models NMDC-T and NMDC-phi on the compactness and mass-radius relation. We find that coupling parameters of NMDC-T is less sensitive than NMDC-phi.

What carries the argument

Direct comparison of coupling-parameter sensitivity between the NMDC-T (stress-energy trace) and NMDC-phi (scalar-field) versions inside the Tolman-Oppenheimer-Volkoff equations for an incompressible fluid.

Load-bearing premise

The two models NMDC-T and NMDC-phi can be directly and fairly compared when applied to an incompressible star, with no hidden inconsistencies in the field equations or boundary conditions that would invalidate the sensitivity comparison.

What would settle it

A explicit numerical solution showing that, for the same range of coupling values and the same incompressible equation of state, the fractional change in compactness or radius is equal or larger in NMDC-T than in NMDC-phi.

Figures

Figures reproduced from arXiv: 2604.04617 by Agus Suroso, Bobby Eka Gunara, Ilham Prasetyo.

Figure 1
Figure 1. Figure 1: Simplified flowchart of the shooting method for NMDC-phi model. [PITH_FULL_IMAGE:figures/full_fig_p005_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: NMDC-phi variation of parameter η > 0. + + + + + + + + + + + + + * * * * * * * * * * * * * + β/κ>0 * β/κ<0 10-11 10-8 10-5 0.01 0.260 0.265 0.270 0.275 |β|/κ GM/R [PITH_FULL_IMAGE:figures/full_fig_p011_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: NMDC-T variation of parameter [PITH_FULL_IMAGE:figures/full_fig_p011_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: MR relation (left) and central pressure vs. compactness relation (right) for NMDC-phi. [PITH_FULL_IMAGE:figures/full_fig_p011_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: MR relation (left) and central pressure vs. compactness relation (right) for NMDC-T. [PITH_FULL_IMAGE:figures/full_fig_p012_5.png] view at source ↗
read the original abstract

In this article, we report the results of comparing the effect of using trace of stress-energy tensor versus real-valued scalar field in Nonminimal Derivative Coupling gravitation model, respectively denoted as NMDC-T and NMDC-phi. We employ the model into an incompressible star and see the effect of both models NMDC-T and NMDC-phi on the compactness and mass-radius relation. We find that coupling parameters of NMDC-T is less sensitive than NMDC-phi.

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 paper compares two variants of the Nonminimal Derivative Coupling (NMDC) model applied to an incompressible star: NMDC-T (coupling to the trace of the stress-energy tensor) versus NMDC-phi (coupling to a real scalar field). It examines the resulting effects on stellar compactness and mass-radius relations and concludes that the coupling parameters in NMDC-T are less sensitive than those in NMDC-phi.

Significance. If the reported difference in parameter sensitivity holds under the stated approximations, the result indicates that NMDC-T may yield more robust predictions for compact-object structure with reduced dependence on the coupling strength. This could be useful for narrowing viable parameter ranges in modified-gravity stellar models, though the preliminary scope and incompressible-fluid assumption limit immediate observational implications.

minor comments (2)
  1. Abstract: the sentence 'We find that coupling parameters of NMDC-T is less sensitive than NMDC-phi' contains a subject-verb agreement error and an incomplete comparison; it should read 'are less sensitive than those of NMDC-phi'.
  2. The manuscript would benefit from a brief statement of the numerical integration method, step size, and convergence criteria used to obtain the mass-radius curves, even if the central comparison is already supported by the field equations.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their review of our manuscript and for recommending minor revision. The referee's summary accurately captures the scope and conclusions of our preliminary comparison between the NMDC-T and NMDC-phi variants applied to incompressible stars. No specific major comments were raised in the report.

read point-by-point responses
  1. Referee: The paper compares two variants of the Nonminimal Derivative Coupling (NMDC) model applied to an incompressible star: NMDC-T versus NMDC-phi. It examines the resulting effects on stellar compactness and mass-radius relations and concludes that the coupling parameters in NMDC-T are less sensitive than those in NMDC-phi.

    Authors: We confirm that this is an accurate description of our work. The numerical results for the compactness and mass-radius relations under the incompressible-fluid assumption indeed show reduced sensitivity of the coupling parameter in the NMDC-T case relative to NMDC-phi. revision: no

  2. Referee: If the reported difference in parameter sensitivity holds under the stated approximations, the result indicates that NMDC-T may yield more robust predictions for compact-object structure with reduced dependence on the coupling strength. This could be useful for narrowing viable parameter ranges in modified-gravity stellar models, though the preliminary scope and incompressible-fluid assumption limit immediate observational implications.

    Authors: We agree that the difference in sensitivity is tied to the approximations used. In the revised manuscript we will add a short paragraph in the conclusions explicitly reiterating that the study is preliminary and that the incompressible-fluid assumption restricts direct observational application, while noting that the reduced parameter sensitivity remains a robust feature within the model assumptions. revision: yes

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper conducts a direct numerical comparison of two model variants (NMDC-T using the trace of the stress-energy tensor and NMDC-phi using a scalar field) by inserting each into the stellar structure equations for an incompressible star and extracting compactness and mass-radius curves. The reported difference in coupling-parameter sensitivity follows from solving those equations under stated boundary conditions (p=0 at the surface, asymptotic flatness) and is not obtained by re-expressing any fitted quantity as a prediction or by invoking a self-citation that itself contains the target result. No equation or step in the supplied text reduces by construction to its own input, so the derivation chain remains independent of the final claim.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only the abstract is available, so no explicit free parameters, axioms, or invented entities can be identified from the provided information.

pith-pipeline@v0.9.0 · 5388 in / 1119 out tokens · 56823 ms · 2026-05-12T02:11:17.716505+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

14 extracted references · 14 canonical work pages

  1. [1]

    Charmousis, E

    C. Charmousis, E. J. Copeland, A. Padilla, and P. M. Saffin,Phys. Rev. D85, 104040 (2012)

  2. [2]

    G. W. Horndeski,Int. J. Theor. Phys.10, 363-384 (1974)

  3. [3]

    Cisterna, T

    A. Cisterna, T. Delsate, and M. Rinaldi,Phys. Rev. D92, no.4, 044050 (2015)

  4. [4]

    Cisterna, T

    A. Cisterna, T. Delsate, L. Ducobu, and M. Rinaldi,Phys. Rev. D93, no.8, 084046 (2016)

  5. [5]

    M. D. Danarianto, I. Prasetyo, A. Suroso, B. E. Gunara, and A. Sulaksono,Phys. Dark Univ.48, 101919 (2025)

  6. [6]

    Hui, and A

    L. Hui, and A. Nicolis,Phys. Rev. Lett.110, 241104 (2013)

  7. [7]

    Rinaldi,Phys

    M. Rinaldi,Phys. Rev. D86, 084048 (2012)

  8. [8]

    Babichev and C

    E. Babichev and C. Charmousis,JHEP08, 106 (2014)

  9. [9]

    Asimakis, S

    P. Asimakis, S. Basilakos, A. Lymperis, M. Petronikolou, and E. N. Saridakis,Phys. Rev. D107, 104006 (2023)

  10. [10]

    J. M. Martin-Garcia et al.xAct: Efficient tensor computer algebra for the Wolfram Language.http://www.xact.es. Accessed: 2025-11-13

  11. [11]

    J. D. Brown,Class. Quant. Grav.10, 1579-1606 (1993)

  12. [12]

    Y. Z. Fan, M. Z. Han, J. L. Jiang, D. S. Shao and S. P. Tang,Phys. Rev. D109, no.4, 043052 (2024)

  13. [13]

    Rezzolla, E

    L. Rezzolla, E. R. Most and L. R. Weih,Astrophys. J. Lett.852, no.2, L25 (2018)

  14. [14]

    B. P. Abbottet al.[LIGO Scientific and Virgo],Phys. Rev. Lett.119, no.16, 161101 (2017)