pith. machine review for the scientific record. sign in

arxiv: 2512.14921 · v2 · submitted 2025-12-16 · 🌀 gr-qc · astro-ph.HE

Recognition: 1 theorem link

· Lean Theorem

ell-Boson stars in anti-de Sitter spacetime

Authors on Pith no claims yet

Pith reviewed 2026-05-16 21:16 UTC · model grok-4.3

classification 🌀 gr-qc astro-ph.HE
keywords ℓ-boson starsanti-de Sitter spacetimeboson starscosmological constantscalar fieldsgeneral relativityasymptotically AdS
0
0 comments X

The pith

ℓ-boson stars admit regular solutions that are asymptotically anti-de Sitter.

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

The paper extends ℓ-boson stars, which generalize standard boson stars by an angular momentum number ℓ while preserving spherical symmetry, to spacetimes with a negative cosmological constant. It shows that the scalar-field and metric ansatz from flat space produces solutions that remain regular everywhere and approach anti-de Sitter geometry at large distances. A reader would care because these configurations provide concrete examples of self-gravitating scalar-field objects in AdS, allowing study of how the cosmological constant affects their mass, size, and other properties. The work examines how the solutions depend on the value of the cosmological constant and on ℓ.

Core claim

ℓ-boson stars, a generalization of standard boson stars parameterized by an angular momentum number ℓ while preserving the spacetime's spherical symmetry, admit regular solutions in spacetimes with a negative cosmological constant such that they are asymptotically anti-de Sitter.

What carries the argument

The ℓ-boson star ansatz: a complex scalar field with harmonic time dependence and angular dependence set by ℓ, inserted into the Einstein equations with a negative cosmological constant term.

If this is right

  • Families of regular, asymptotically AdS solutions exist for a range of ℓ values and cosmological constants.
  • The solutions reduce to the previously known flat-space ℓ-boson stars when the cosmological constant is taken to zero.
  • Global quantities such as total mass and Noether charge can be computed and plotted as functions of the frequency and the cosmological constant.
  • The construction demonstrates that the spherical symmetry of the metric is preserved for any ℓ.

Where Pith is reading between the lines

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

  • The same ansatz approach could be tested for other matter models or for rotating generalizations inside AdS.
  • These solutions might serve as initial data for numerical simulations of gravitational collapse or boson-star mergers in AdS.
  • Stability properties could be examined by linear perturbation analysis around the obtained background metrics.

Load-bearing premise

The same scalar-field ansatz and metric form that worked in flat space continue to yield regular, asymptotically AdS solutions when the cosmological constant is negative.

What would settle it

A numerical solution of the resulting ordinary differential equations that either becomes singular at finite radius or fails to approach the anti-de Sitter metric at infinity would show that such stars do not exist.

Figures

Figures reproduced from arXiv: 2512.14921 by Miguel Megevand.

Figure 1
Figure 1. Figure 1: FIG. 1. Field profiles for [PITH_FULL_IMAGE:figures/full_fig_p006_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Density profiles for [PITH_FULL_IMAGE:figures/full_fig_p007_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Total mass [PITH_FULL_IMAGE:figures/full_fig_p007_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Compactness of maximum mass solutions vs. [PITH_FULL_IMAGE:figures/full_fig_p008_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Types of circular orbits for solutions with [PITH_FULL_IMAGE:figures/full_fig_p008_5.png] view at source ↗
read the original abstract

In previous work, we introduced the $\ell$-boson stars, a generalization of standard boson stars, which are parameterized by an angular momentum number $\ell$, while still preserving the spacetime's spherical symmetry. In this article, we present and study the properties of $\ell$-boson stars in spacetimes with a negative cosmological constant, such that they are asymptotically anti-de Sitter.

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 / 2 minor

Summary. The manuscript extends the ℓ-boson star construction—spherically symmetric solutions sourced by a complex scalar field with angular momentum quantum number ℓ—to asymptotically anti-de Sitter spacetime. It solves the Einstein-scalar system with negative cosmological constant numerically and reports families of regular solutions whose properties are studied as functions of ℓ and the AdS radius.

Significance. If the numerical solutions are shown to be asymptotically AdS and free of singularities, the work supplies a concrete set of boson-star configurations in AdS that could serve as backgrounds for holographic studies or as probes of the AdS/CFT dictionary. The extension from Minkowski to AdS is incremental but useful provided the asymptotics and regularity are rigorously verified.

major comments (1)
  1. [Method / Ansatz and Numerical Setup] The central construction re-uses the flat-space ℓ-boson-star ansatz (scalar field with angular dependence averaged to spherical symmetry, metric functions A(r), B(r), δ(r)). With Λ < 0 the Einstein-scalar equations acquire an extra curvature term, and asymptotic AdS requires A(r) → 1 + r²/L² together with the appropriate scalar fall-off. The manuscript does not explicitly demonstrate how the shooting parameters are adjusted to satisfy these boundary conditions at infinity while preserving regularity at r = 0; this step is load-bearing for the existence claim.
minor comments (2)
  1. The abstract and introduction should state the precise boundary conditions imposed at spatial infinity and at the origin, together with any convergence tests or error estimates for the numerical solutions.
  2. Figures showing the metric functions and scalar profiles should include the asymptotic AdS behavior explicitly (e.g., comparison with 1 + r²/L²) to allow direct visual verification.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for the constructive comment on the numerical construction. We address the point raised below and will revise the text to make the boundary-condition procedure fully explicit.

read point-by-point responses
  1. Referee: The central construction re-uses the flat-space ℓ-boson-star ansatz (scalar field with angular dependence averaged to spherical symmetry, metric functions A(r), B(r), δ(r)). With Λ < 0 the Einstein-scalar equations acquire an extra curvature term, and asymptotic AdS requires A(r) → 1 + r²/L² together with the appropriate scalar fall-off. The manuscript does not explicitly demonstrate how the shooting parameters are adjusted to satisfy these boundary conditions at infinity while preserving regularity at r = 0; this step is load-bearing for the existence claim.

    Authors: We agree that an explicit description of the shooting procedure is necessary for the AdS case. In the revised manuscript we will insert a dedicated paragraph (new subsection 3.2) that details the numerical method: the system is integrated outward from r = 0 using regularity conditions A(0) = 1, B(0) = 1, δ(0) = 0 and vanishing first derivatives of the scalar field; a two-parameter shooting algorithm then tunes the central scalar amplitude and the frequency parameter so that, at large r, A(r) − (1 + r²/L²) falls below a prescribed tolerance and the scalar field exhibits the expected AdS fall-off. We will also add representative plots of the metric functions and their asymptotic residuals, together with convergence tests under grid refinement, to confirm that the reported families are indeed regular and asymptotically AdS. revision: yes

Circularity Check

1 steps flagged

Minor self-citation to prior flat-space work; AdS solutions obtained independently via field equations

specific steps
  1. self citation load bearing [Abstract]
    "In previous work, we introduced the ℓ-boson stars, a generalization of standard boson stars, which are parameterized by an angular momentum number ℓ, while still preserving the spacetime's spherical symmetry. In this article, we present and study the properties of ℓ-boson stars in spacetimes with a negative cosmological constant, such that they are asymptotically anti-de Sitter."

    The opening sentence anchors the new AdS study in the authors' own prior definition of the ℓ-boson star ansatz. While this is a normal citation practice and does not force the AdS solutions by construction, it is the only self-referential element; the numerical construction of regular asymptotically-AdS solutions proceeds from the field equations rather than from any redefinition or fit internal to the present paper.

full rationale

The paper extends the ℓ-boson star construction to negative cosmological constant by solving the Einstein-scalar equations with the same ansatz for the scalar field and metric functions. No evidence that any reported property is defined in terms of fitted parameters from the same dataset or that the central result reduces to a self-citation chain. The self-citation to the authors' prior introduction of ℓ-boson stars is present but supplies only the starting ansatz; the AdS asymptotics and regularity are enforced by the modified equations and boundary conditions, which constitute independent content.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The construction rests on the Einstein equations with negative cosmological constant, a minimally coupled complex scalar field, and the same spherically symmetric ansatz used in flat space. No new entities are postulated.

axioms (2)
  • standard math Einstein equations with negative cosmological constant hold
    Invoked to obtain the metric-scalar system in AdS
  • domain assumption Complex scalar field is minimally coupled and the ℓ-harmonic ansatz preserves spherical symmetry
    Carried over from the authors' previous flat-space paper

pith-pipeline@v0.9.0 · 5345 in / 1216 out tokens · 39423 ms · 2026-05-16T21:16:50.066237+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

79 extracted references · 79 canonical work pages · 29 internal anchors

  1. [1]

    2 0 π 4 π 2 0 0.1 1 10 ∞ µ= 0 A ψ δ ℓ= 0 ℓ= 1 ℓ= 2 ℓ= 3 ℓ= 4 ℓ= 5 ℓ= 6 A, ψ, δ x r/L FIG. 1. Field profiles forµ= 0 in the maximum mass cases. boundary. This is because those solutions were obtained numerically using the non-compact formulation, setting a boundary at finite, but large enough values ofr. However, those curves can be easily extended using t...

  2. [2]

    6 0 π 4 π 2 0 0.1 1 10 ∞ µ = 0

  3. [3]

    242 0 0 . 05 0 . 1 0 . 15 0 . 2 0 0 . 05 0 . 1 0 . 15 0 . 2 ℓ = 0 ℓ = 1 ℓ = 2 ℓ = 3 ℓ = 4 ℓ = 5 ℓ = 6 L2ρ x r/L FIG. 2. Density profiles forµ= 0 in the maximum mass cases. 0

  4. [4]

    7 2 3 4 5 6 7 8 9 ← u 0 µ = 0, ℓ = 0 1 2 3 4 5 6 Lµ = 1, ℓ = 0 1 2 3 4 5 6 M/L L ωℓ FIG. 3. Total massMvs frequencyω ℓ forµ= 0 andLµ= 1. In order to compare solutions with different values ofℓ, we decide to concentrate on the particular solutions with the maximum mass. Fig. 4 shows how the compactness increases withℓ. This fact might not be obvious since ...

  5. [5]

    45 0 2 4 6 8 10 12 14 ℓ-boson star limit ( Λ = 0 ) Buchdahl limit Cm, µ = 0 Lµ = 1 C99, µ = 0 Lµ = 1 C ℓ FIG. 4. Compactness of maximum mass solutions vs.ℓ. rlr rm r99

  6. [6]

    27 0 . 28 0 . 29 0 . 3 0 . 31 0 . 32 0 . 33 0 . 34 0 . 35 0 . 36 r/L Cm µ = 0 ℓ = 10 stable circular orbits unstable circular orbits no circular orbits ↑ first region ↓ second region FIG. 5. Types of circular orbits for solutions withµ= 0 andℓ= 10. that, contrary to the case with Λ = 0, solutions with light ring pairs exist in the first region. Forℓ≥4 (not...

  7. [7]

    D. J. Kaup, Klein-Gordon Geon, Phys. Rev.172, 1331 (1968)

  8. [8]

    Ruffini and S

    R. Ruffini and S. Bonazzola, Systems of selfgravitating particles in general relativity and the concept of an equation of state, Phys. Rev.187, 1767 (1969)

  9. [9]

    Colpi, S

    M. Colpi, S. L. Shapiro, and I. Wasserman, Boson Stars: Gravitational Equilibria of Selfinteracting Scalar Fields, Phys. Rev. Lett.57, 2485 (1986)

  10. [10]

    Friedberg, T

    R. Friedberg, T. D. Lee, and Y. Pang, MINI - SOLITON STARS, Phys. Rev. D35, 3640 (1987)

  11. [11]

    Gleiser, Stability of Boson Stars, Phys

    M. Gleiser, Stability of Boson Stars, Phys. Rev. D38, 2376 (1988), [Erratum: Phys.Rev.D 39, 1257 (1989)]

  12. [12]

    T. D. Lee and Y. Pang, Stability of Mini - Boson Stars, Nucl. Phys. B315, 477 (1989)

  13. [13]

    Seidel and W.-M

    E. Seidel and W.-M. Suen, Dynamical Evolution of Boson Stars. 1. Perturbing the Ground State, Phys. Rev. D42, 384 (1990)

  14. [14]

    A. R. Liddle and M. S. Madsen, The Structure and formation of boson stars, Int. J. Mod. Phys. D1, 101 (1992)

  15. [15]

    Jetzer, Boson stars, Phys

    P. Jetzer, Boson stars, Phys. Rept.220, 163 (1992)

  16. [16]

    E. W. Mielke and F. E. Schunck, Boson stars: Early history and recent prospects, in8th Marcel Grossmann Meeting on Recent Developments in Theoretical and Experimental General Relativity, Gravitation and Relativistic Field Theories (MG 8)(1997) pp. 1607–1626, arXiv:gr-qc/9801063

  17. [17]

    F. E. Schunck and E. W. Mielke, General relativistic boson stars, Class. Quant. Grav.20, R301 (2003), arXiv:0801.0307 [astro-ph]

  18. [18]

    E. W. Mielke, Rotating Boson Stars, Fundam. Theor. Phys.183, 115 (2016)

  19. [19]

    Visinelli, Boson stars and oscillatons: A review, Int

    L. Visinelli, Boson stars and oscillatons: A review, Int. J. Mod. Phys. D30, 2130006 (2021), arXiv:2109.05481 [gr-qc]

  20. [20]

    Shnir, Boson Stars, Lect

    Y. Shnir, Boson Stars, Lect. Notes Phys.1017, 347 (2023), arXiv:2204.06374 [gr-qc]

  21. [21]

    S. L. Liebling and C. Palenzuela, Dynamical boson stars, Living Rev. Rel.26, 1 (2023), arXiv:1202.5809 [gr-qc]

  22. [22]

    Sin, Late time cosmological phase transition and galactic halo as Bose liquid, Phys

    S.-J. Sin, Late time cosmological phase transition and galactic halo as Bose liquid, Phys. Rev. D50, 3650 (1994), arXiv:hep- ph/9205208

  23. [23]

    Cosmic Structure as the Quantum Interference of a Coherent Dark Wave

    H.-Y. Schive, T. Chiueh, and T. Broadhurst, Cosmic Structure as the Quantum Interference of a Coherent Dark Wave, Nature Phys.10, 496 (2014), arXiv:1406.6586 [astro-ph.GA]

  24. [24]

    Alcubierre, J

    M. Alcubierre, J. Barranco, A. Bernal, J. C. Degollado, A. Diez-Tejedor, M. Megevand, D. N´ u˜ nez, and O. Sarbach, Gravitational atoms beyond the test field limit: the case of Sgr A* and ultralight dark matter, Class. Quant. Grav.42, 21LT01 (2025), arXiv:2411.18601 [gr-qc]

  25. [25]

    Alcubierre, J

    M. Alcubierre, J. Barranco, A. Bernal, J. C. Degollado, A. Diez-Tejedor, M. Megevand, D. Nunez, and O. Sarbach, Noble gravitational atoms: Self-gravitating black hole scalar wigs with angular momentum number, (2025), arXiv:2512.08095 [gr-qc]

  26. [26]

    Dilute and dense axion stars

    L. Visinelli, S. Baum, J. Redondo, K. Freese, and F. Wilczek, Dilute and dense axion stars, Phys. Lett. B777, 64 (2018), arXiv:1710.08910 [astro-ph.CO]

  27. [27]

    Dense Axion Stars

    E. Braaten, A. Mohapatra, and H. Zhang, Dense Axion Stars, Phys. Rev. Lett.117, 121801 (2016), arXiv:1512.00108 [hep-ph]

  28. [28]

    Guerra, C

    D. Guerra, C. F. B. Macedo, and P. Pani, Axion boson stars, JCAP09(09), 061, [Erratum: JCAP 06, E01 (2020)], arXiv:1909.05515 [gr-qc]

  29. [29]

    R. D. Peccei and H. R. Quinn, CP Conservation in the Presence of Instantons, Phys. Rev. Lett.38, 1440 (1977)

  30. [30]

    Wilczek, Problem of StrongPandTInvariance in the Presence of Instantons, Phys

    F. Wilczek, Problem of StrongPandTInvariance in the Presence of Instantons, Phys. Rev. Lett.40, 279 (1978)

  31. [31]

    Weinberg, A New Light Boson?, Phys

    S. Weinberg, A New Light Boson?, Phys. Rev. Lett.40, 223 (1978)

  32. [32]

    Sikivie, Axion dark matter, Nucl

    P. Sikivie, Axion dark matter, Nucl. Phys. B1003, 116500 (2024)

  33. [33]

    D. F. Torres, S. Capozziello, and G. Lambiase, A Supermassive scalar star at the galactic center?, Phys. Rev. D62, 104012 (2000), arXiv:astro-ph/0004064

  34. [34]

    F. S. Guzman, Accretion disc onto boson stars: A Way to supplant black holes candidates, Phys. Rev. D73, 021501 (2006), arXiv:gr-qc/0512081

  35. [35]

    Constraining scalar fields with stellar kinematics and collisional dark matter

    P. Amaro-Seoane, J. Barranco, A. Bernal, and L. Rezzolla, Constraining scalar fields with stellar kinematics and collisional dark matter, JCAP11, 002, arXiv:1009.0019 [astro-ph.CO]

  36. [36]

    Testing the nature of dark compact objects: a status report

    V. Cardoso and P. Pani, Testing the nature of dark compact objects: a status report, Living Rev. Rel.22, 4 (2019), arXiv:1904.05363 [gr-qc]

  37. [37]

    G. A. Marks, S. J. Staelens, T. Evstafyeva, and U. Sperhake, Long-Term Stable Nonlinear Evolutions of Ultracompact Black-Hole Mimickers, Phys. Rev. Lett.135, 131402 (2025), arXiv:2504.17775 [gr-qc]

  38. [38]

    Astefanesei and E

    D. Astefanesei and E. Radu, Boson stars with negative cosmological constant, Nucl. Phys. B665, 594 (2003), arXiv:gr- qc/0309131

  39. [39]

    Spinning scalar solitons in anti-de Sitter spacetime

    E. Radu and B. Subagyo, Spinning scalar solitons in anti-de Sitter spacetime, Phys. Lett. B717, 450 (2012), arXiv:1207.3715 [gr-qc]

  40. [40]

    Boson Stars in AdS

    A. Buchel, S. L. Liebling, and L. Lehner, Boson stars in AdS spacetime, Phys. Rev. D87, 123006 (2013), arXiv:1304.4166 12 [gr-qc]

  41. [41]

    A comment on "Boson stars in AdS"

    M. Maliborski and A. Rostworowski, A comment on ”Boson stars in AdS”, arXive (2013), arXiv:1307.2875 [gr-qc]

  42. [42]

    Self-interacting boson stars with a single Killing vector field in Anti-de Sitter

    Y. Brihaye, B. Hartmann, and J. Riedel, Self-interacting boson stars with a single Killing vector field in anti–de Sitter space-time, Phys. Rev. D92, 044049 (2015), arXiv:1404.1874 [gr-qc]

  43. [43]

    Self-gravitating scalar breathers with negative cosmological constant

    G. Fodor, P. Forg´ acs, and P. Grandcl´ ement, Self-gravitating scalar breathers with negative cosmological constant, Phys. Rev. D92, 025036 (2015), arXiv:1503.07746 [gr-qc]

  44. [44]

    P. T. Chru´ sciel, E. Delay, P. Klinger, A. Kriegl, P. W. Michor, and A. Rainer, Non-singular space-times with a negative cosmological constant: V. Boson stars, Lett. Math. Phys.108, 2009 (2018), arXiv:1708.02878 [gr-qc]

  45. [45]

    H.-S. Liu, H. Lu, and Y. Pang, Revisiting the AdS Boson Stars: the Mass-Charge Relations, Phys. Rev. D102, 126008 (2020), arXiv:2007.15017 [hep-th]

  46. [46]

    Guo, H.-S

    S.-F. Guo, H.-S. Liu, H. L¨ u, and Y. Pang, Large-charge limit of AdS boson stars with mixed boundary conditions, JHEP 04, 220, arXiv:2101.00017 [hep-th]

  47. [47]

    Herdeiro, H

    C. Herdeiro, H. Huang, J. Kunz, and E. Radu, Einstein-(complex)-Maxwell static boson stars in AdS, Phys. Lett. B856, 138939 (2024), arXiv:2405.10671 [gr-qc]

  48. [48]

    Liu, Y.-Q

    S.-C. Liu, Y.-Q. Wang, and Z.-H. Zhao, Frozen solitonic Hayward-boson stars in Anti-de Sitter Spacetime, (2025), arXiv:2512.10197 [gr-qc]

  49. [49]

    Zhao, Y.-N

    Z.-H. Zhao, Y.-N. Gu, S.-C. Liu, Z.-Q. Liu, and Y.-Q. Wang, Light Rings, Accretion Disks and Shadows of Hayward Boson Stars in asymptotically AdS Spacetime, (2025), arXiv:2507.09563 [gr-qc]

  50. [50]

    S. W. Hawking and G. F. R. Ellis,The Large Scale Structure of Space-Time, Cambridge Monographs on Mathematical Physics (Cambridge University Press, 1973)

  51. [51]

    Nonlinear Evolution and Final Fate of Charged Anti-de Sitter Black Hole Superradiant Instability

    P. Bosch, S. R. Green, and L. Lehner, Nonlinear Evolution and Final Fate of Charged Anti–de Sitter Black Hole Superra- diant Instability, Phys. Rev. Lett.116, 141102 (2016), arXiv:1601.01384 [gr-qc]

  52. [52]

    P. Basu, C. Krishnan, and P. N. Bala Subramanian, Hairy Black Holes in a Box, JHEP11, 041, arXiv:1609.01208 [hep-th]

  53. [53]

    Studies of a general flat space/boson star transition model in a box through a language similar to holographic superconductors

    Y. Peng, Studies of a general flat space/boson star transition model in a box through a language similar to holographic superconductors, JHEP07, 042, arXiv:1705.08694 [hep-th]

  54. [54]

    Y. Peng, B. Wang, and Y. Liu, On the thermodynamics of the black hole and hairy black hole transitions in the asymp- totically flat spacetime with a box, Eur. Phys. J. C78, 176 (2018), arXiv:1708.01411 [hep-th]

  55. [55]

    H. R. C. Ferreira and C. A. R. Herdeiro, Superradiant instabilities in the Kerr-mirror and Kerr-AdS black holes with Robin boundary conditions, Phys. Rev. D97, 084003 (2018), arXiv:1712.03398 [gr-qc]

  56. [56]

    Anti De Sitter Space And Holography

    E. Witten, Anti de Sitter space and holography, Adv. Theor. Math. Phys.2, 253 (1998), arXiv:hep-th/9802150

  57. [57]

    J. M. Maldacena, The LargeNlimit of superconformal field theories and supergravity, Adv. Theor. Math. Phys.2, 231 (1998), arXiv:hep-th/9711200

  58. [58]

    On weakly turbulent instability of anti-de Sitter space

    P. Bizon and A. Rostworowski, On weakly turbulent instability of anti-de Sitter space, Phys. Rev. Lett.107, 031102 (2011), arXiv:1104.3702 [gr-qc]

  59. [59]

    Ja lmu˙ zna, A

    J. Ja lmu˙ zna, A. Rostworowski, and P. Bizo´ n, Ads collapse of a scalar field in higher dimensions, Phys. Rev. D84, 085021 (2011)

  60. [60]

    Scalar Collapse in AdS

    A. Buchel, L. Lehner, and S. L. Liebling, Scalar Collapse in AdS, Phys. Rev. D86, 123011 (2012), arXiv:1210.0890 [gr-qc]

  61. [61]

    O. J. C. Dias, G. T. Horowitz, D. Marolf, and J. E. Santos, On the Nonlinear Stability of Asymptotically Anti-de Sitter Solutions, Class. Quant. Grav.29, 235019 (2012), arXiv:1208.5772 [gr-qc]

  62. [62]

    Alcubierre, J

    M. Alcubierre, J. Barranco, A. Bernal, J. C. Degollado, A. Diez-Tejedor, M. Megevand, D. Nunez, and O. Sarbach,ℓ-Boson stars, Class. Quant. Grav.35, 19LT01 (2018), arXiv:1805.11488 [gr-qc]

  63. [63]

    Alcubierre, J

    M. Alcubierre, J. Barranco, A. Bernal, J. C. Degollado, A. Diez-Tejedor, M. Megevand, D. N´ u˜ nez, and O. Sarbach, Boson stars and their relatives in semiclassical gravity, Phys. Rev. D107, 045017 (2023), arXiv:2212.02530 [gr-qc]

  64. [64]

    Alcubierre, J

    M. Alcubierre, J. Barranco, A. Bernal, J. C. Degollado, A. Diez-Tejedor, V. Jaramillo, M. Megevand, D. N´ u˜ nez, and O. Sarbach, Extremeℓ-boson stars, Class. Quant. Grav.39, 094001 (2022), arXiv:2112.04529 [gr-qc]

  65. [65]

    Alcubierre, J

    M. Alcubierre, J. Barranco, A. Bernal, J. C. Degollado, A. Diez-Tejedor, M. Megevand, D. N´ u˜ nez, and O. Sarbach, On the linear stability ofℓ-boson stars with respect to radial perturbations, Class. Quant. Grav.38, 174001 (2021), arXiv:2103.15012 [gr-qc]

  66. [66]

    Alcubierre, J

    M. Alcubierre, J. Barranco, A. Bernal, J. C. Degollado, A. Diez-Tejedor, M. Megevand, D. N´ u˜ nez, and O. Sarbach, Dynamical evolutions ofℓ-boson stars in spherical symmetry, Class. Quant. Grav.36, 215013 (2019), arXiv:1906.08959 [gr-qc]

  67. [67]

    Jaramillo, N

    V. Jaramillo, N. Sanchis-Gual, J. Barranco, A. Bernal, J. C. Degollado, C. Herdeiro, and D. N´ u˜ nez, Dynamicalℓ-boson stars: Generic stability and evidence for nonspherical solutions, Phys. Rev. D101, 124020 (2020), arXiv:2004.08459 [gr-qc]

  68. [68]

    Jaramillo, N

    V. Jaramillo, N. Sanchis-Gual, J. Barranco, A. Bernal, J. C. Degollado, C. Herdeiro, M. Megevand, and D. N´ u˜ nez, Head-on collisions ofℓ-boson stars, Phys. Rev. D105, 104057 (2022), arXiv:2202.00696 [gr-qc]

  69. [69]

    R. M. Wald,General Relativity(University of Chicago Press, Chicago, U.S.A., 1984)

  70. [70]

    P. V. P. Cunha, E. Berti, and C. A. R. Herdeiro, Light-Ring Stability for Ultracompact Objects, Phys. Rev. Lett.119, 251102 (2017), arXiv:1708.04211 [gr-qc]

  71. [71]

    M. Guo, Z. Zhong, J. Wang, and S. Gao, Light rings and long-lived modes in quasiblack hole spacetimes, Phys. Rev. D 105, 024049 (2022), arXiv:2108.08967 [gr-qc]

  72. [72]

    Peng, No-go theorem for static boson stars with negative cosmological constants, Nucl

    Y. Peng, No-go theorem for static boson stars with negative cosmological constants, Nucl. Phys. B953, 114955 (2020), arXiv:1902.06508 [gr-qc]

  73. [73]

    W. H. Press, S. A. Teukolsky, W. T. Vetterling, and B. P. Flannery,Numerical Recipes in FORTRAN: The Art of Scientific Computing, 2nd ed. (Cambridge University Press, Cambridge, 1992). 13

  74. [74]

    Radhakrishnan and A

    K. Radhakrishnan and A. C. Hindmarsh,Description and use of LSODE, the Livermore solver for ordinary differential equations, LLNL report UCRL-ID-113855 (Lawrence Livermore National Laboratory, 1993)

  75. [75]

    Scalar field confinement as a model for accreting systems

    M. Megevand, I. Olabarrieta, and L. Lehner, Scalar field confinement as a model for accreting systems, Class. Quant. Grav. 24, 3235 (2007), arXiv:0705.0644 [gr-qc]

  76. [76]

    Dynamical Evolution of Boson Stars II: Excited States and Self-Interacting Fields

    J. Balakrishna, E. Seidel, and W.-M. Suen, Dynamical evolution of boson stars. 2. Excited states and selfinteracting fields, Phys. Rev. D58, 104004 (1998), arXiv:gr-qc/9712064

  77. [77]

    Multi-state Boson Stars

    A. Bernal, J. Barranco, D. Alic, and C. Palenzuela, Multi-state Boson Stars, Phys. Rev. D81, 044031 (2010), arXiv:0908.2435 [gr-qc]

  78. [78]

    H. A. Buchdahl, General Relativistic Fluid Spheres, Phys. Rev.116, 1027 (1959)

  79. [79]

    Barranco, J

    J. Barranco, J. Chagoya, A. Diez-Tejedor, G. Niz, and A. A. Roque, Horndeski stars, JCAP10, 022, arXiv:2108.01679 [gr-qc]