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arxiv: 2607.00840 · v1 · pith:F7Z5PMENnew · submitted 2026-07-01 · ✦ hep-ph · astro-ph.HE

Dark matter energy exchange in stars orbiting supermassive black holes

Pith reviewed 2026-07-02 09:58 UTC · model grok-4.3

classification ✦ hep-ph astro-ph.HE
keywords dark matterenergy exchangestellar orbitssupermassive black holesdark starsscattering cross sectionsgalactic centerfreeze-in
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0 comments X

The pith

Dark matter scattering can match the luminosity of stars orbiting close to supermassive black holes at cross sections of 10^{-36} cm² for a spiked density profile.

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

The paper calculates the average energy a star gains from scattering off dark matter particles during its orbit around the galactic center black hole. For the star S4714 on a very close orbit, this energy input equals the star's luminosity when the dark matter density is spiked and the scattering cross section is around 10^{-36} cm² for MeV to GeV dark matter masses or 5×10^{-38} cm² for lighter masses. This matters to a sympathetic reader because it shows a way stars could become dark stars through energy transfer alone, without dark matter annihilating inside them. The required cross sections fit models where dark matter is produced by freeze-in and do not violate other bounds from cosmic rays or the sun.

Core claim

Stars on tight orbits around the supermassive black hole at the Galactic Center pass through regions where the dark matter density may be strongly enhanced. For a spiked dark matter profile, the exchange reaches the stellar luminosity at σ_χp ∼ 10^{-36} cm² for MeV-GeV masses and σ_χe ∼ 5×10^{-38} cm² for sub-MeV masses, opening a new annihilation-free route toward dark-star phases. These cross sections lie within the range predicted by freeze-in scenarios and are consistent with cosmic-ray-boosted and solar-reflection dark matter constraints.

What carries the argument

The orbit-averaged DM-induced energy exchange rate computed for a star on a relativistic orbit in a spiked dark matter density profile.

If this is right

  • The energy exchange can reach the level of the star's own luminosity.
  • This occurs at cross sections compatible with freeze-in dark matter production.
  • The values remain consistent with constraints from cosmic-ray boosted dark matter and solar reflection.
  • Stars can reach dark-star phases without requiring dark matter annihilation.

Where Pith is reading between the lines

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

  • If the spiked profile is present, measurements of stellar energy output near galactic centers could constrain dark matter scattering cross sections.
  • The mechanism could be tested by comparing predicted and observed luminosities for other known close-orbit stars.
  • Applying this to different galactic centers might reveal similar effects if spikes form there too.

Load-bearing premise

The dark matter density near the supermassive black hole is enhanced in a spiked profile that the star's orbit samples.

What would settle it

Observation or modeling that the dark matter density profile around Sagittarius A* does not have a strong enough spike to make the energy exchange match luminosity at the stated cross sections.

Figures

Figures reproduced from arXiv: 2607.00840 by Ian M. Shoemaker, Jayden L. Newstead, Nicole F. Bell, R. Andrew Gustafson, Sandra Robles, Stephan A. Meighen-Berger.

Figure 1
Figure 1. Figure 1: FIG. 1. Schematic illustration of a star on a highly eccentric [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. DM density as a function of radius. The pink band [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Analytic orbit-averaged DM–proton energy ex [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Analytic orbit-averaged DM-induced energy exchange [PITH_FULL_IMAGE:figures/full_fig_p005_6.png] view at source ↗
read the original abstract

Stars on tight orbits around the supermassive black hole at the Galactic Center pass through regions where the dark matter~(DM) density may be strongly enhanced. We compute the orbit-averaged DM-induced energy exchange for S4714 as an example. It is a star on an exceptionally close and relativistic orbit around Sagittarius~A*. For a spiked dark matter profile, the exchange reaches the stellar luminosity at $\sigma_{\chi p} \sim 10^{-36}~\mathrm{cm}^2$ for MeV-GeV masses and $\sigma_{\chi e} \sim 5\times10^{-38}~\mathrm{cm}^2$ for sub-MeV masses, opening a new annihilation-free route toward dark-star phases. These cross sections lie within the range predicted by freeze-in scenarios and are consistent with cosmic-ray--boosted and solar-reflection dark matter constraints.

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 manuscript computes the orbit-averaged energy exchange rate between dark matter and the star S4714 on its close, relativistic orbit around Sagittarius A*. For an assumed spiked DM density profile, the exchange equals stellar luminosity at σ_χp ∼ 10^{-36} cm² (MeV-GeV masses) and σ_χe ∼ 5×10^{-38} cm² (sub-MeV masses), framing this as an annihilation-free channel toward dark-star phases that lies inside freeze-in and cosmic-ray-boosted constraints.

Significance. If the modeling assumptions hold, the result identifies a new astrophysical signature of DM scattering near SMBHs that connects laboratory-accessible cross sections to observable stellar properties, without invoking annihilation. No machine-checked proofs or public code are reported, but the forward calculation from standard profiles and orbital data is a clear strength.

major comments (2)
  1. [DM profile modeling (abstract and profile section)] The spiked DM density profile is load-bearing for the central claim that the quoted cross sections reach L_star. Without a quantitative sensitivity study showing how the required σ values shift for a non-spiked (e.g., NFW or adiabatically contracted but non-spiked) profile at ∼10^{-3} pc, the result cannot be assessed as lying inside the freeze-in window.
  2. [Energy exchange calculation] The orbit-averaged energy-exchange formula and its numerical evaluation (including integration limits, DM velocity distribution, and relativistic corrections for S4714) are not visible in sufficient detail to verify the quoted cross-section thresholds; this prevents confirmation that the luminosity-matching values are robust.
minor comments (1)
  1. [Abstract] The abstract states the cross sections without quoting the exact spike parameters (e.g., power-law index or normalization radius) used; a one-sentence definition or reference would improve clarity.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the detailed and constructive report. We address each major comment below. Where revisions are needed to improve clarity and robustness, we will incorporate them in the revised manuscript.

read point-by-point responses
  1. Referee: [DM profile modeling (abstract and profile section)] The spiked DM density profile is load-bearing for the central claim that the quoted cross sections reach L_star. Without a quantitative sensitivity study showing how the required σ values shift for a non-spiked (e.g., NFW or adiabatically contracted but non-spiked) profile at ∼10^{-3} pc, the result cannot be assessed as lying inside the freeze-in window.

    Authors: The spiked profile is the physically motivated case for the Galactic Center due to adiabatic contraction from SMBH growth, as standard in the literature for such orbits. For non-spiked profiles the DM density drops sharply and the required cross sections would increase substantially, potentially outside the freeze-in window; our claim is therefore scoped to the spiked scenario as a possible new signature. We will add a short quantitative sensitivity paragraph (including order-of-magnitude estimates for NFW and contracted non-spiked cases at the relevant radii) to make this dependence explicit. revision: yes

  2. Referee: [Energy exchange calculation] The orbit-averaged energy-exchange formula and its numerical evaluation (including integration limits, DM velocity distribution, and relativistic corrections for S4714) are not visible in sufficient detail to verify the quoted cross-section thresholds; this prevents confirmation that the luminosity-matching values are robust.

    Authors: We agree that additional detail is required for reproducibility. The orbit average is obtained by integrating the local energy-transfer rate (using the standard DM-star scattering kinematics) along the relativistic orbit of S4714, with the DM velocity distribution taken as isotropic in the spike frame and relativistic corrections applied to the relative velocity and energy transfer. We will insert the explicit integral expression, the adopted integration limits, the form of the velocity distribution, and the treatment of relativistic effects into the methods section of the revised manuscript. revision: yes

Circularity Check

0 steps flagged

No circularity; forward calculation from external profile assumption

full rationale

The derivation computes orbit-averaged energy exchange rates from an input spiked DM density profile, S4714 orbital data, and scattering cross sections, then compares the result to stellar luminosity to obtain required sigma values. No equations reduce outputs to fitted inputs by construction, no self-citations are load-bearing for the central result, and the spiked profile is invoked as a modeling choice rather than derived internally. The calculation is self-contained against external benchmarks and does not exhibit any of the enumerated circular patterns.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the unverified assumption of a spiked DM density profile near Sgr A* and standard stellar parameters for S4714; no free parameters or invented entities are explicitly introduced in the abstract.

axioms (1)
  • domain assumption Dark matter density follows a spiked profile near the supermassive black hole
    Required to reach the luminosity-matching cross sections quoted in the abstract.

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discussion (0)

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Reference graph

Works this paper leans on

71 extracted references · 66 canonical work pages · 38 internal anchors

  1. [1]

    SINFONI in the Galactic Center: young stars and IR flares in the central light month

    F. Eisenhaueret al., SINFONI in the Galactic Center: Young stars and IR flares in the central light month, As- trophys. J.628, 246 (2005), arXiv:astro-ph/0502129

  2. [2]

    On the nature of the fast moving star S2 in the Galactic Center

    F. Martins, S. Gillessen, F. Eisenhauer, R. Genzel, T. Ott, and S. Trippe, On the nature of the fast mov- ing star S2 in the Galactic Center, Astrophys. J. Lett. 672, L119 (2008), arXiv:0711.3344 [astro-ph]

  3. [3]

    Detection of the gravitational redshift in the orbit of the star S2 near the Galactic centre massive black hole

    R. Abuteret al.(GRAVITY), Detection of the gravita- tional redshift in the orbit of the star S2 near the Galactic centre massive black hole, Astron. Astrophys.615, L15 (2018), arXiv:1807.09409 [astro-ph.GA]

  4. [4]

    Peißker, A

    F. Peißker, A. Eckart, M. Zajaˇ cek, B. Ali, and M. Parsa, S62 and S4711: Indications of a Population of Faint Fast-moving Stars inside the S2 Orbit—S4711 on a 7.6 yr Orbit around Sgr A*, Astrophys. J.899, 50 (2020), arXiv:2008.04764 [astro-ph.GA]

  5. [5]

    Dark matter annihilation at the galactic center

    P. Gondolo and J. Silk, Dark matter annihilation at the galactic center, Phys. Rev. Lett.83, 1719 (1999), arXiv:astro-ph/9906391

  6. [6]

    G. D. Quinlan, L. Hernquist, and S. Sigurdsson, Models of Galaxies with Central Black Holes: Adiabatic Growth in Spherical Galaxies, Astrophys. J.440, 554 (1995), arXiv:astro-ph/9407005

  7. [7]

    Dark matter distributions around massive black holes: A general relativistic analysis

    L. Sadeghian, F. Ferrer, and C. M. Will, Dark mat- ter distributions around massive black holes: A general relativistic analysis, Phys. Rev. D88, 063522 (2013), arXiv:1305.2619 [astro-ph.GA]

  8. [8]

    Time-Dependent Models for Dark Matter at the Galactic Center

    G. Bertone and D. Merritt, Time-dependent models for dark matter at the Galactic Center, Phys. Rev. D72, 103502 (2005), arXiv:astro-ph/0501555

  9. [9]

    Dark Matter Dynamics and Indirect Detection

    G. Bertone and D. Merritt, Dark matter dynamics and indirect detection, Mod. Phys. Lett. A20, 1021 (2005), arXiv:astro-ph/0504422

  10. [10]

    Balaji, D

    S. Balaji, D. Sachdeva, F. Sala, and J. Silk, Dark mat- ter spikes around Sgr A* inγ-rays, JCAP08, 063, arXiv:2303.12107 [hep-ph]

  11. [11]

    Akita, A

    K. Akita, A. Ibarra, and R. Zimmermann, Dark matter explanations for the neutrino emission from the Seyfert galaxy NGC 1068, arXiv:2507.16539 [hep-ph] (2025)

  12. [12]

    Dynamical constraints on a dark matter spike at the Galactic Centre from stellar orbits

    T. Lacroix, Dynamical constraints on a dark matter spike at the Galactic Centre from stellar orbits, Astron. Astro- phys.619, A46 (2018), arXiv:1801.01308 [astro-ph.GA]

  13. [13]

    Abd El Dayemet al.(GRAVITY), Improving con- straints on the extended mass distribution in the Galactic center with stellar orbits, Astron

    K. Abd El Dayemet al.(GRAVITY), Improving con- straints on the extended mass distribution in the Galactic center with stellar orbits, Astron. Astrophys.692, A242 (2024), arXiv:2409.12261 [astro-ph.GA]

  14. [14]

    Dark stars at the Galactic centre - the main sequence

    P. Scott, M. Fairbairn, and J. Edsjo, Dark stars at the Galactic centre - the main sequence, Mon. Not. Roy. As- tron. Soc.394, 82 (2009), arXiv:0809.1871 [astro-ph]

  15. [15]

    I. John, R. K. Leane, and T. Linden, Dark matter scattering constraints from observations of stars sur- rounding Sgr A*, Phys. Rev. D109, 123041 (2024), arXiv:2311.16228 [astro-ph.HE]

  16. [16]

    J. F. Acevedo, A. J. Reilly, and L. Santos-Olmsted, Dark Drag Around Sagittarius A* (2025), arXiv:2510.01320 [hep-ph]

  17. [17]

    R. A. Gustafson, I. M. Shoemaker, and V. Takhistov, Probing Dark Matter Interactions with Stellar Motion near Sagittarius A* (2025), arXiv:2510.07387 [hep-ph]

  18. [18]

    G. Elor, R. McGehee, and A. Pierce, Maximizing Di- rect Detection with Highly Interactive Particle Relic Dark Matter, Phys. Rev. Lett.130, 031803 (2023), arXiv:2112.03920 [hep-ph]

  19. [19]

    P. N. Bhattiprolu, G. Elor, R. McGehee, and A. Pierce, Freezing-in hadrophilic dark matter at low reheating tem- peratures, JHEP01, 128, arXiv:2210.15653 [hep-ph]

  20. [20]

    J. F. Navarro, C. S. Frenk, and S. D. M. White, The Structure of cold dark matter halos, Astrophys. J.462, 563 (1996), arXiv:astro-ph/9508025

  21. [21]

    PPPC 4 DM ID: A Poor Particle Physicist Cookbook for Dark Matter Indirect Detection

    M. Cirelli, G. Corcella, A. Hektor, G. Hutsi, M. Kadastik, P. Panci, M. Raidal, F. Sala, and A. Strumia, PPPC 4 DM ID: A Poor Particle Physicist Cookbook for Dark Matter Indirect Detection, JCAP03, 051, [Erratum: JCAP 10, E01 (2012)], arXiv:1012.4515 [hep-ph]

  22. [22]

    O. Y. Gnedin and J. R. Primack, Dark Matter Profile in the Galactic Center, Phys. Rev. Lett.93, 061302 (2004), arXiv:astro-ph/0308385

  23. [23]

    Made-to-Measure models of the Galactic Box/Peanut bulge: stellar and total mass in the bulge region

    M. Portail, C. Wegg, O. Gerhard, and I. Martinez- Valpuesta, Made-to-measure models of the Galactic box/peanut bulge: stellar and total mass in the bulge region, Monthly Notices of the Royal Astronomical Soci- ety448, 713 (2015), arXiv:1502.00633 [astro-ph.GA]

  24. [24]

    An estimate of the DM profile in the Galactic bulge region

    F. Iocco and M. Benito, An estimate of the DM profile in the Galactic bulge region, Phys. Dark Univ.15, 90 (2017), arXiv:1611.09861 [astro-ph.GA]

  25. [25]

    The Density of Dark Matter in the Galactic Bulge and Implications for Indirect Detection

    D. Hooper, The Density of Dark Matter in the Galac- tic Bulge and Implications for Indirect Detection, Phys. Dark Univ.15, 53 (2017), arXiv:1608.00003 [astro- ph.HE]

  26. [26]

    Baumgart, S

    M. Baumgart, S. Bottaro, D. Redigolo, N. L. Rodd, and T. R. Slatyer, Testing real WIMPs with CTAO, JHEP 02, 213, arXiv:2507.15937 [hep-ph]

  27. [27]

    T. K. Karydas, F. Scarcella, B. J. Kavanagh, and G. Bertone, On the survival of dark matter spikes: Stellar and compact-object perturbations (2026), arXiv:2606.13761 [astro-ph.GA]

  28. [28]

    Gould, Resonant enhancements in wimp capture by the earth, Astrophys

    A. Gould, Resonant enhancements in wimp capture by the earth, Astrophys. J.321, 571 (1987)

  29. [29]

    Gould, WIMP Distribution in and Evaporation From the Sun, Astrophys

    A. Gould, WIMP Distribution in and Evaporation From the Sun, Astrophys. J.321, 560 (1987)

  30. [30]

    Modules for Experiments in Stellar Astrophysics (MESA)

    B. Paxton, L. Bildsten, A. Dotter, F. Herwig, P. Lesaffre, and F. Timmes, Modules for Experiments in Stellar As- trophysics (MESA), Astrophysical Journal Supplement Series192, 3 (2011), arXiv:1009.1622 [astro-ph.SR]

  31. [31]

    Modules for Experiments in Stellar Astrophysics (MESA): Giant Planets, Oscillations, Rotation, and Massive Stars

    B. Paxton, M. Cantiello, P. Arras, L. Bildsten, E. F. Brown, A. Dotter, C. Mankovich, M. H. Montgomery, D. Stello, F. X. Timmes, and R. Townsend, Modules for Experiments in Stellar Astrophysics (MESA): Plan- ets, Oscillations, Rotation, and Massive Stars, The As- trophysical Journal Supplement Series208, 4 (2013), arXiv:1301.0319 [astro-ph.SR]

  32. [32]

    Modules for Experiments in Stellar Astrophysics (MESA): Binaries, Pulsations, and Explosions

    B. Paxton, P. Marchant, J. Schwab, E. B. Bauer, L. Bild- sten, M. Cantiello, L. Dessart, R. Farmer, H. Hu, N. Langer, R. H. D. Townsend, D. M. Townsley, and F. X. Timmes, Modules for Experiments in Stellar Astro- physics (MESA): Binaries, Pulsations, and Explosions, 11 The Astrophysical Journal Supplement Series220, 15 (2015), arXiv:1506.03146 [astro-ph.SR]

  33. [33]

    Modules for Experiments in Stellar Astrophysics (MESA): Convective Boundaries, Element Diffusion, and Massive Star Explosions

    B. Paxtonet al., Modules for Experiments in Stellar Astrophysics (MESA): Convective Boundaries, Element Diffusion, and Massive Star Explosions, Astrophys. J. Suppl.234, 34 (2018), arXiv:1710.08424 [astro-ph.SR]

  34. [34]

    Modules for Experiments in Stellar Astrophysics (MESA): Pulsating Variable Stars, Rotation, Convective Boundaries, and Energy Conservation

    B. Paxton, R. Smolec, J. Schwab, A. Gautschy, L. Bild- sten, M. Cantiello, A. Dotter, R. Farmer, J. A. Goldberg, A. S. Jermyn, S. M. Kanbur, P. Marchant, A. Thoul, R. H. D. Townsend, W. M. Wolf, M. Zhang, and F. X. Timmes, Modules for Experiments in Stellar As- trophysics (MESA): Pulsating Variable Stars, Rotation, Convective Boundaries, and Energy Conser...

  35. [35]

    A. S. Jermynet al.(MESA), Modules for Experiments in Stellar Astrophysics (MESA): Time-dependent Convec- tion, Energy Conservation, Automatic Differentiation, and Infrastructure, Astrophys. J. Suppl.265, 15 (2023), arXiv:2208.03651 [astro-ph.SR]

  36. [36]

    Aalberset al.(LZ), New Constraints on Cos- mic Ray-Boosted Dark Matter from the LUX-ZEPLIN Experiment, Phys

    J. Aalberset al.(LZ), New Constraints on Cos- mic Ray-Boosted Dark Matter from the LUX-ZEPLIN Experiment, Phys. Rev. Lett.134, 241801 (2025), arXiv:2503.18158 [hep-ex]

  37. [37]

    Direct detection of dark matter—APPEC committee report*,

    J. Billardet al., Direct detection of dark matter—appec committee report*, Rept. Prog. Phys.85, 056201 (2022), arXiv:2104.07634 [hep-ex]

  38. [38]

    Results on MeV-scale dark matter from a gram-scale cryogenic calorimeter operated above ground

    G. Angloheret al.(CRESST), Results on MeV-scale dark matter from a gram-scale cryogenic calorimeter op- erated above ground, Eur. Phys. J. C77, 637 (2017), arXiv:1707.06749 [astro-ph.CO]

  39. [39]

    Angloheret al.(CRESST), Testing spin-dependent dark matter interactions with lithium aluminate tar- gets in CRESST-III, Phys

    G. Angloheret al.(CRESST), Testing spin-dependent dark matter interactions with lithium aluminate tar- gets in CRESST-III, Phys. Rev. D106, 092008 (2022), arXiv:2207.07640 [astro-ph.CO]

  40. [40]

    Aguilar-Arevaloet al.(DAMIC), Results on low-mass weakly interacting massive particles from a 11 kg-day target exposure of DAMIC at SNOLAB, Phys

    A. Aguilar-Arevaloet al.(DAMIC), Results on low-mass weakly interacting massive particles from a 11 kg-day target exposure of DAMIC at SNOLAB, Phys. Rev. Lett. 125, 241803 (2020), arXiv:2007.15622 [astro-ph.CO]

  41. [41]

    Low-Mass Dark Matter Search with the DarkSide-50 Experiment

    P. Agneset al.(DarkSide), Low-Mass Dark Mat- ter Search with the DarkSide-50 Experiment, Phys. Rev. Lett.121, 081307 (2018), arXiv:1802.06994 [astro- ph.HE]

  42. [42]

    DarkSide-50 532-day Dark Matter Search with Low-Radioactivity Argon

    P. Agneset al.(DarkSide), DarkSide-50 532-day Dark Matter Search with Low-Radioactivity Argon, Phys. Rev. D98, 102006 (2018), arXiv:1802.07198 [astro-ph.CO]

  43. [43]

    Dark Matter Search Results from a One Tonne$\times$Year Exposure of XENON1T

    E. Aprileet al.(XENON), Dark Matter Search Results from a One Ton-Year Exposure of XENON1T, Phys. Rev. Lett.121, 111302 (2018), arXiv:1805.12562 [astro- ph.CO]

  44. [44]

    Aprileet al.(XENON), Light Dark Matter Search with Ionization Signals in XENON1T, Phys

    E. Aprileet al.(XENON), Light Dark Matter Search with Ionization Signals in XENON1T, Phys. Rev. Lett. 123, 251801 (2019), arXiv:1907.11485 [hep-ex]

  45. [45]

    Sabti, J

    N. Sabti, J. Alvey, M. Escudero, M. Fairbairn, and D. Blas, Refined Bounds on MeV-scale Thermal Dark Sectors from BBN and the CMB, JCAP01, 004, arXiv:1910.01649 [hep-ph]

  46. [46]

    Krnjaic and S

    G. Krnjaic and S. D. McDermott, Implications of BBN Bounds for Cosmic Ray Upscattered Dark Matter, Phys. Rev. D101, 123022 (2020), arXiv:1908.00007 [hep-ph]

  47. [47]

    Sabti, J

    N. Sabti, J. Alvey, M. Escudero, M. Fairbairn, and D. Blas, Addendum: Refined bounds on MeV-scale ther- mal dark sectors from BBN and the CMB, JCAP08, A01, arXiv:2107.11232 [hep-ph]

  48. [48]

    E. O. Nadler, V. Gluscevic, K. K. Boddy, and R. H. Wechsler, Constraints on Dark Matter Microphysics from the Milky Way Satellite Population, Astrophys. J. Lett.878, 32 (2019), [Erratum: Astrophys.J.Lett. 897, L46 (2020), Erratum: Astrophys.J. 897, L46 (2020)], arXiv:1904.10000 [astro-ph.CO]

  49. [49]

    H. An, H. Nie, M. Pospelov, J. Pradler, and A. Ritz, Solar reflection of dark matter, Phys. Rev. D104, 103026 (2021), arXiv:2108.10332 [hep-ph]

  50. [50]

    Zhanget al.(PandaX), Search for Light Dark Matter with 259 Days of Data in PandaX-4T, Phys

    M. Zhanget al.(PandaX), Search for Light Dark Matter with 259 Days of Data in PandaX-4T, Phys. Rev. Lett. 135, 211001 (2025), arXiv:2507.11930 [hep-ex]

  51. [51]

    New Constraints and Prospects for sub-GeV Dark Matter Scattering off Electrons in Xenon

    R. Essig, T. Volansky, and T.-T. Yu, New Constraints and Prospects for sub-GeV Dark Matter Scattering off Electrons in Xenon, Phys. Rev. D96, 043017 (2017), arXiv:1703.00910 [hep-ph]

  52. [52]

    Dark matter and the first stars: a new phase of stellar evolution

    D. Spolyar, K. Freese, and P. Gondolo, Dark matter and the first stars: a new phase of stellar evolution, Phys. Rev. Lett.100, 051101 (2008), arXiv:0705.0521 [astro- ph]

  53. [53]

    Dark Matter capture and annihilation on the First Stars: preliminary estimates

    F. Iocco, Dark Matter Capture and Annihilation on the First Stars: Preliminary Estimates, Astrophys. J. Lett. 677, L1 (2008), arXiv:0802.0941 [astro-ph]

  54. [54]

    I. V. Moskalenko and L. Wai, Dark matter burners: Pre- liminary estimates (2006), arXiv:astro-ph/0608535

  55. [55]

    Dark Stars: A Review

    K. Freese, T. Rindler-Daller, D. Spolyar, and M. Valluri, Dark Stars: A Review, Rept. Prog. Phys.79, 066902 (2016), arXiv:1501.02394 [astro-ph.CO]

  56. [56]

    Peißker, A

    F. Peißker, A. Eckart, M. Zajaˇ cek, and S. Britzen, Obser- vation of S4716-a Star with a 4 yr Orbit around Sgr A*, Astrophys. J.933, 49 (2022), arXiv:2207.02142 [astro- ph.GA]

  57. [57]

    Abuteret al.(GRAVITY), Astron

    R. Abuteret al.(GRAVITY), Mass distribution in the Galactic Center based on interferometric astrometry of multiple stellar orbits, Astron. Astrophys.657, L12 (2022), arXiv:2112.07478 [astro-ph.GA]

  58. [58]

    King’s College London, King’s Computational Research, Engineering and Technology Environment (CREATE) (2026)

  59. [59]

    The Galactic Center Massive Black Hole and Nuclear Star Cluster

    R. Genzel, F. Eisenhauer, and S. Gillessen, The Galac- tic Center massive black hole and nuclear star cluster, Rev. Mod. Phys.82, 3121 (2010), arXiv:1006.0064 [astro- ph.GA]

  60. [60]

    The structure of the nuclear stellar cluster of the Milky Way

    R. Schodelet al., The structure of the nuclear stellar cluster of the Milky Way (2007), arXiv:astro-ph/0703178

  61. [61]

    The nuclear star cluster of the Milky Way

    R. Schoedel, D. Merritt, and A. Eckart, The nuclear star cluster of the Milky Way, J. Phys. Conf. Ser.131, 012044 (2008), arXiv:0810.0204 [astro-ph]

  62. [62]

    F. K. Baganoffet al., Chandra x-ray spectroscopic imag- ing of Sgr A* and the central parsec of the Galaxy, As- trophys. J.591, 891 (2003), arXiv:astro-ph/0102151

  63. [63]

    P. G. Mezger, W. J. Duschl, and R. Zylka, The Galactic Center: a laboratory for AGN?, Astronomy and Astro- physics Review7, 289 (1996)

  64. [64]

    Betancourt Kamenetskaia, M

    B. Betancourt Kamenetskaia, M. Fujiwara, A. Ibarra, and T. Toma, Dark matter spikes with strongly self- interacting particles, JCAP09, 074, arXiv:2506.12642 [hep-ph]

  65. [65]

    D. N. Spergel and P. J. Steinhardt, Observational ev- idence for selfinteracting cold dark matter, Phys. Rev. Lett.84, 3760 (2000), arXiv:astro-ph/9909386

  66. [66]

    Dark Matter Halos as Particle Colliders: A Unified Solution to Small-Scale Structure Puzzles from Dwarfs to Clusters

    M. Kaplinghat, S. Tulin, and H.-B. Yu, Dark Matter Halos as Particle Colliders: Unified Solution to Small- Scale Structure Puzzles from Dwarfs to Clusters, Phys. 12 Rev. Lett.116, 041302 (2016), arXiv:1508.03339 [astro- ph.CO]

  67. [67]

    Zhang and Y

    Z.-C. Zhang and Y. Tang, Velocity distribution of dark matter in spikes around Schwarzschild black holes and effects on gravitational waves from extreme-mass- ratio inspirals, Phys. Rev. D110, 103008 (2024), arXiv:2403.18529 [astro-ph.GA]

  68. [68]

    Zhang, H.-C

    Z.-C. Zhang, H.-C. Yuan, and Y. Tang, Universal den- sity and velocity distributions of dark matter around massive black holes, Phys. Rev. D112, 043025 (2025), arXiv:2503.02573 [astro-ph.GA]

  69. [69]

    A. K. Drukier, K. Freese, and D. N. Spergel, Detecting Cold Dark Matter Candidates, Phys. Rev. D33, 3495 (1986)

  70. [70]

    Twelve years of spectroscopic monitoring in the Galactic Center: the closest look at S-stars near the black hole

    M. Habibi, S. Gillessen, F. Martins, F. Eisenhauer, P. M. Plewa, O. Pfuhl, E. George, J. Dexter, I. Waisberg, T. Ott, S. von Fellenberg, M. Baub¨ ock, A. Jimenez- Rosales, and R. Genzel, Twelve Years of Spectroscopic Monitoring in the Galactic Center: The Closest Look at S-stars near the Black Hole, Astrophys. J.847, 120 (2017), arXiv:1708.06353 [astro-ph.SR]

  71. [71]

    The GWs from the S-stars revolving around the SMBH at Sgr A*

    R.-G. Cai, T.-B. Liu, and S.-J. Wang, Gws from s- stars revolving around smbh at sgr a**, Commun. Theor. Phys.70, 735 (2018), arXiv:1808.03164 [gr-qc]