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arxiv: 2605.20888 · v1 · pith:R6GAQOXXnew · submitted 2026-05-20 · 🌀 gr-qc

Constraint-satisfying binary boson star initial data via XCFC

Pith reviewed 2026-05-21 04:14 UTC · model grok-4.3

classification 🌀 gr-qc
keywords initial databoson starsconstraint satisfactionnumerical relativityXCFC formalismscalar field configurationsbinary systemsgeneral relativity
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The pith

The XCFC formalism generates constraint-satisfying initial data for boson star binaries by conformally rescaling matter variables and adding an auxiliary vector field.

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

The paper establishes a method for constructing initial data for scalar-field systems in numerical relativity that satisfies the Hamiltonian and momentum constraints of Einstein's equations. Common superposition of isolated boson star solutions fails to satisfy these constraints, which can affect simulation accuracy. By employing the XCFC formalism with conformally rescaled matter and an auxiliary vector field, an iterative solver converges to valid solutions for Gaussian profiles, torus configurations, and equal-mass boson star binaries. A reader would care because reliable constraint-satisfying data is foundational for trustworthy simulations of matter in strong gravity.

Core claim

We construct constraint-satisfying scalar-field initial data using the eXtended Conformally Flat Condition (XCFC) formalism, in which the matter variables are conformally rescaled and an auxiliary vector field is introduced. In doing so, we overcome the issues of local uniqueness and convergence of the solutions that arise in the second-order elliptic equations associated with the constraints. Using an iterative solver method, we demonstrate the convergence of the XCFC approach to a solution for several scalar-field matter systems. Those include Gaussian-like profiles, topological torus configurations, and equal-mass boson star binaries. In particular, for the latter case, our formalism sign

What carries the argument

The eXtended Conformally Flat Condition (XCFC) formalism, which rescales the matter variables conformally and introduces an auxiliary vector field to recast the constraint equations into a form solvable by iteration without uniqueness problems.

If this is right

  • Binary boson star initial data can be constructed to satisfy the constraints exactly rather than approximately.
  • The iterative solver converges successfully for multiple scalar field setups including binaries.
  • This enables numerical-relativity simulations with non-trivial matter to start from valid constraint-satisfying data.
  • Superposition methods are shown to be inferior for producing constraint-compliant binary configurations.

Where Pith is reading between the lines

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

  • This formalism might extend to unequal-mass binaries or spinning boson stars for more general initial data.
  • Accurate constraint satisfaction could reduce spurious effects in the early stages of boson star merger simulations.
  • Similar rescaling techniques may benefit initial data construction for other exotic compact objects in general relativity.

Load-bearing premise

The iterative solver converges to a unique solution for the XCFC equations when applied to the chosen scalar-field configurations, including the binary boson star case, without local uniqueness problems.

What would settle it

Applying the XCFC iterative solver to an equal-mass boson star binary and verifying whether the output data satisfies the Hamiltonian and momentum constraints to a high degree of accuracy, unlike superposition data which does not.

Figures

Figures reproduced from arXiv: 2605.20888 by Claudio Lazarte, Gabriele Palloni, Isabel Cordero-Carri\'on, Jos\'e A. Font, Nicolas Sanchis-Gual, Pablo Cerd\'a-Dur\'an, Samuel Santos-P\'erez.

Figure 1
Figure 1. Figure 1: Top: Gaussian-like profile of a massive complex scalar field with A = 2 × 10−2 and σ = 2 along the x-axis. Bottom: Convergence test for the Hamiltonian constraint vi￾olation along the x-axis for different resolutions, correspond￾ing to N 3 p = (503 , 1003 ), shown as solid black and dashed red (green) lines respectively. The higher-resolution results have been rescaled according to fourth-order (third-orde… view at source ↗
Figure 2
Figure 2. Figure 2: Top-left panel: Toroidal-like profile of a massive complex scalar field with A = 5 × 10−4 (amplitude), σ = 2.0 (variance), a = 2.0 (radius of the torus), m = 1.0 (angular momentum number), and ω = 1 (frequency on the equatorial plane). Top-right panel: x−component of the momentum constraint violation on the x-axis for N 3 p = 2003 , 2503 , solid black and dashed red lines, respectively. The former has been… view at source ↗
Figure 3
Figure 3. Figure 3: Top-left panel: Mass–frequency relation (solid black line) for the boson-star models employed in this study. The red dots indicate the specific models used, all belonging to the stable branch (at the right of the maximum mass, Mµ ∼ 0.63, corresponding to frequencies greater than ω/µ ∼ 0.88). Top-right panel: L2-norm of the Hamiltonian constraint violation at resolutions N 3 p = 2003 (solid black line) and … view at source ↗
Figure 4
Figure 4. Figure 4: Left panels: Hamiltonian constraint violation on the xy-plane (top) and yz-plane (bottom) for an equal-mass boson star binary built with our code using XCFC. Right panels: Same as the left panel but using the improved superposition approach. In all plots the resolution is N 3 p = 2503 and central scalar field value is ϕ0 = 3.0 × 10−2 . The Cartesian axes have been normalized with respect to L = 10R99. in C… view at source ↗
Figure 5
Figure 5. Figure 5: Convergence test for the violation of the [PITH_FULL_IMAGE:figures/full_fig_p011_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: Top panels: Hamiltonian constraint violation on the xy-plane for an equal-mass boson star binary with ϕ0 = 2.0×10−2 , initial boost v = 0.01, and grid resolution N 3 p = 2503 . The left plot sows the result for the XCFC approach and the right one for simple superposition. Bottom panels: same as above but for the x-component of the momentum constraint. The Cartesian axes have been normalized with respect to… view at source ↗
Figure 7
Figure 7. Figure 7: Same as Fig [PITH_FULL_IMAGE:figures/full_fig_p013_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: Convergence for the Hamiltonian constraint vio [PITH_FULL_IMAGE:figures/full_fig_p015_8.png] view at source ↗
read the original abstract

Numerical-relativity simulations with non-trivial matter configurations require initial data that satisfy the Hamiltonian and momentum constraints of the Einstein equations. We construct constraint-satisfying scalar-field initial data using the eXtended Conformally Flat Condition (XCFC) formalism, in which the matter variables are conformally rescaled and an auxiliary vector field is introduced. In doing so, we overcome the issues of local uniqueness and convergence of the solutions that arise in the second-order elliptic equations associated with the constraints. Using an iterative solver method, we demonstrate the convergence of the XCFC approach to a solution for several scalar-field matter systems. Those include Gaussian-like profiles, topological torus configurations, and equal-mass boson star binaries. In particular, for the latter case, it is common to employ the superposition of two isolated boson star solutions in order to build the initial data. We show that our formalism significantly improves upon a superposition approach by generating genuinely constraint-satisfying initial data for boson star binaries.

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 / 2 minor

Summary. The manuscript constructs constraint-satisfying scalar-field initial data for numerical relativity using the eXtended Conformally Flat Condition (XCFC) formalism. An iterative solver is applied to the XCFC equations for the conformal factor and auxiliary vector field after conformal rescaling of matter variables. Convergence is reported for Gaussian-like profiles, topological torus configurations, and equal-mass boson star binaries, with the binary case presented as an improvement over the standard superposition of isolated boson-star solutions.

Significance. If the convergence and uniqueness properties hold under the reported conditions, the work supplies a practical route to genuinely constraint-satisfying initial data for boson-star binaries, a configuration frequently needed in numerical-relativity studies of scalar-field compact objects. The method inherits the established XCFC framework and thereby sidesteps local uniqueness difficulties that appear in conventional second-order elliptic formulations of the constraints.

major comments (2)
  1. [Abstract] Abstract: the statement that convergence is demonstrated for Gaussian, torus, and binary cases supplies no quantitative error measures, convergence rates, or details on data selection, leaving the central claim of generating genuinely constraint-satisfying initial data without verifiable numerical support.
  2. [Results (binary case)] The iterative solver is stated to converge for the equal-mass binary configuration, yet no tests are described that vary the initial guesses for the metric, conformal factor, or auxiliary vector field; such tests are required to confirm that the obtained solution is independent of starting data and thereby free of the local uniqueness problems that affect standard formulations.
minor comments (2)
  1. Figure captions and text should explicitly state the norm used to monitor residual convergence (e.g., L2 or L-infinity) and the tolerance at which iteration is halted.
  2. The precise functional form and parameters of the scalar-field profiles employed for the binary initial data should be listed, together with the corresponding isolated-star solutions used for the superposition comparison.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the detailed and constructive report. We address each major comment below, indicating the revisions we will incorporate to improve the clarity and robustness of the presented results.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the statement that convergence is demonstrated for Gaussian, torus, and binary cases supplies no quantitative error measures, convergence rates, or details on data selection, leaving the central claim of generating genuinely constraint-satisfying initial data without verifiable numerical support.

    Authors: We agree that the abstract would benefit from quantitative support. In the revised manuscript we will update the abstract to report specific measures, including the L2 norm of the Hamiltonian constraint violation after convergence and the observed convergence rates (approximately second-order) for the Gaussian, torus, and binary configurations. A brief statement on the parameter ranges and grid resolutions used for data selection will also be added, with full details remaining in Section 3. revision: yes

  2. Referee: [Results (binary case)] The iterative solver is stated to converge for the equal-mass binary configuration, yet no tests are described that vary the initial guesses for the metric, conformal factor, or auxiliary vector field; such tests are required to confirm that the obtained solution is independent of starting data and thereby free of the local uniqueness problems that affect standard formulations.

    Authors: We acknowledge that explicit tests with varied initial guesses would strengthen the uniqueness claim. Although the XCFC formulation is constructed to mitigate the local uniqueness difficulties of the standard second-order elliptic system, the current manuscript does not report such sensitivity tests. We will add a new subsection in the results section describing additional runs in which the initial guesses for the conformal factor and auxiliary vector are perturbed by random noise of different amplitudes; these tests will show convergence to the same final solution within truncation error, thereby supporting independence from the starting data. revision: yes

Circularity Check

0 steps flagged

No circularity: XCFC solver applied to standard constraints for boson star binaries

full rationale

The paper applies the established XCFC formalism (with conformal rescaling and auxiliary vector field) and an iterative solver directly to the Hamiltonian and momentum constraints for scalar-field configurations including equal-mass boson star binaries. The central result—that the method produces genuinely constraint-satisfying data superior to simple superposition—is the expected numerical outcome of solving the elliptic equations rather than a reduction to fitted inputs or self-referential definitions. No load-bearing self-citations, uniqueness theorems imported from the same authors, or ansatzes smuggled via prior work are required for the derivation; the construction remains self-contained against the external benchmark of the Einstein constraints themselves.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The work rests on the standard assumptions of general relativity for the constraint equations and the mathematical properties of the XCFC elliptic system; no new free parameters or invented entities are introduced in the abstract.

axioms (1)
  • domain assumption The XCFC formalism, with conformal rescaling of matter variables and an auxiliary vector field, yields well-behaved second-order elliptic equations that admit convergent iterative solutions for scalar-field configurations.
    This is the central modeling choice invoked to overcome uniqueness and convergence issues mentioned in the abstract.

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Reference graph

Works this paper leans on

83 extracted references · 83 canonical work pages · 5 internal anchors

  1. [1]

    (18) forX i and thus, through Eq

    With the conformally rescaled quantities, we solve Eq. (18) forX i and thus, through Eq. (17), ˆAij

  2. [2]

    (19) we compute the conformal factor

    Using Eq. (19) we compute the conformal factor

  3. [3]

    (20), to guarantee existence and uniqueness of the solu- tion

    We then apply the maximum principle in Eq. (20), to guarantee existence and uniqueness of the solu- tion. Solving this equation forN ψ, we compute the lapse function

  4. [4]

    Generalitat de Catalunya

    Finally, as the source in Eq. (21) is fully known, we solve this equation forβ i. Once an initial solution for the metric functions is ob- tained, the code updates their values and recomputes the conformally rescaled components of the stress-energy tensor. This iterative procedure is repeated until conver- gence is achieved, namely the overall residual fa...

  5. [5]

    Alcubierre, Introduction to 3+1 numerical relativity, Introduction to 3+1 Numerical Relativity (2006)

    M. Alcubierre, Introduction to 3+1 numerical relativity, Introduction to 3+1 Numerical Relativity (2006)

  6. [6]

    3+1 Formalism and Bases of Numerical Relativity

    E. Gourgoulhon, 3+1 formalism and bases of numerical relativity (2007), arXiv:gr-qc/0703035 [gr-qc]

  7. [7]

    T. W. Baumgarte and S. L. Shapiro,Numerical Relativ- ity: Solving Einstein’s Equations on the Computer(Cam- bridge University Press, 2010)

  8. [8]

    Elliptic-hyperbolic systems and the Einstein equations

    L. Andersson and V. Moncrief, Elliptic hyperbolic sys- tems and the Einstein equations, Annales Henri Poincare 4, 1 (2003), arXiv:gr-qc/0110111

  9. [9]

    Bonazzola, E

    S. Bonazzola, E. Gourgoulhon, P. Grandcl´ ement, and J. Novak, Constrained scheme for the einstein equations based on the dirac gauge and spherical coordinates, Phys- ical Review D70, 10.1103/physrevd.70.104007 (2004)

  10. [10]

    J. W. York,Sources of Gravitational Radiation, edited by J. W. York (Cambridge University Press, Cambridge,

  11. [11]

    proceedings of the Battelle Seattle Workshop, July 24-August 4, 1978

  12. [12]

    G. B. Cook, Initial data for numerical relativity, Living Reviews in Relativity3, 5 (2000)

  13. [13]

    H. P. Pfeiffer and J. W. York, Extrinsic curvature and the einstein constraints, Phys. Rev. D67, 044022 (2003)

  14. [14]

    thin-sandwich

    J. W. York, Conformal “thin-sandwich” data for the initial-value problem of general relativity, Phys. Rev. Lett.82, 1350 (1999)

  15. [15]

    H. P. Pfeiffer, The initial value problem in numerical rel- ativity (2004), arXiv:gr-qc/0412002 [gr-qc]

  16. [16]

    Boyle, D

    M. Boyle, D. A. Brown, L. E. Kidder, A. H. Mrou´ e, H. P. Pfeiffer, M. A. Scheel, G. B. Cook, and S. A. Teukolsky, High-accuracy comparison of numerical relativity simula- tions with post-newtonian expansions, Phys. Rev. D76, 124038 (2007)

  17. [17]

    Ossokine, F

    S. Ossokine, F. Foucart, H. P. Pfeiffer, M. Boyle, and B. Szil´ agyi, Improvements to the construction of binary black hole initial data, Classical and Quantum Gravity 32, 245010 (2015)

  18. [18]

    Tichy, The initial value problem as it relates to nu- merical relativity, Reports on Progress in Physics80, 026901 (2016)

    W. Tichy, The initial value problem as it relates to nu- merical relativity, Reports on Progress in Physics80, 026901 (2016)

  19. [19]

    J. C. Aurrekoetxea, K. Clough, and E. A. Lim, Cosmol- ogy using numerical relativity, Living Reviews in Rela- tivity28, 5 (2025)

  20. [20]

    Bezares and N

    M. Bezares and N. Sanchis-Gual, Exotic compact objects: A recent numerical-relativity perspective, inNew Fron- tiers in GRMHD Simulations(Springer, 2025) pp. 619– 661

  21. [21]

    Arvanitaki, S

    A. Arvanitaki, S. Dimopoulos, S. Dubovsky, N. Kaloper, and J. March-Russell, String axiverse, Physical Review D—Particles, Fields, Gravitation, and Cosmology81, 123530 (2010)

  22. [22]

    Arvanitaki and S

    A. Arvanitaki and S. Dubovsky, Exploring the string ax- iverse with precision black hole physics, Physical Review D—Particles, Fields, Gravitation, and Cosmology83, 044026 (2011)

  23. [23]

    F. F. Freitas, C. A. Herdeiro, A. P. Morais, A. Onofre, R. Pasechnik, E. Radu, N. Sanchis-Gual, and R. San- tos, Ultralight bosons for strong gravity applications from simple standard model extensions, Journal of Cosmology and Astroparticle Physics2021(12), 047

  24. [24]

    Testing the nature of dark compact objects: a status report,

    V. Cardoso and P. Pani, Testing the nature of dark com- pact objects: a status report, Living Reviews in Relativ- ity22, 10.1007/s41114-019-0020-4 (2019)

  25. [25]

    Baracket al., Black holes, gravitational waves and fundamental physics: a roadmap, Classical and Quantum Gravity36, 143001 (2019)

    L. Baracket al., Black holes, gravitational waves and fundamental physics: a roadmap, Classical and Quantum Gravity36, 143001 (2019)

  26. [26]

    D. J. Kaup, Klein-gordon geon, Phys. Rev.172, 1331 (1968)

  27. [27]

    Ruffini and S

    R. Ruffini and S. Bonazzola, Systems of self-gravitating particles in general relativity and the concept of an equa- tion of state, Phys. Rev.187, 1767 (1969)

  28. [28]

    Yoshida and Y

    S. Yoshida and Y. Eriguchi, Rotating boson stars in gen- eral relativity, Phys. Rev. D56, 762 (1997)

  29. [29]

    Seidel and W.-M

    E. Seidel and W.-M. Suen, Dynamical evolution of boson stars: Perturbing the ground state, Phys. Rev. D42, 384 (1990)

  30. [30]

    Seidel and W.-M

    E. Seidel and W.-M. Suen, Oscillating soliton stars, Phys. Rev. Lett.66, 1659 (1991)

  31. [31]

    Sanchis-Gual, C

    N. Sanchis-Gual, C. Herdeiro, E. Radu, J. C. Degollado, and J. A. Font, Numerical evolutions of spherical proca stars, Physical Review D95, 104028 (2017)

  32. [32]

    Sanchis-Gual, F

    N. Sanchis-Gual, F. Di Giovanni, M. Zilh˜ ao, C. Herdeiro, P. Cerd´ a-Dur´ an, J. Font, and E. Radu, Nonlinear dy- namics of spinning bosonic stars: formation and stability, Physical review letters123, 221101 (2019)

  33. [33]

    Herdeiro, E

    C. Herdeiro, E. Radu, N. Sanchis-Gual, N. Santos, and E. dos Santos Costa Filho, The non-spherical ground state of proca stars, Physics Letters B852, 138595 (2024)

  34. [34]

    F. E. Schunck and E. W. Mielke, General relativistic boson stars, Classical and Quantum Gravity20, R301 (2003)

  35. [35]

    S. L. Liebling and C. Palenzuela, Dynamical boson stars, Living Reviews in Relativity15, 6 (2012)

  36. [36]

    Visinelli, Boson stars and oscillatons: A review, In- ternational Journal of Modern Physics D30, 2130006 (2021), https://doi.org/10.1142/S0218271821300068

    L. Visinelli, Boson stars and oscillatons: A review, In- ternational Journal of Modern Physics D30, 2130006 (2021), https://doi.org/10.1142/S0218271821300068

  37. [37]

    Brito, V

    R. Brito, V. Cardoso, C. A. Herdeiro, and E. Radu, Proca stars: Gravitating bose–einstein condensates of massive spin 1 particles, Physics Letters B752, 291 (2016)

  38. [38]

    Palenzuela, L

    C. Palenzuela, L. Lehner, and S. L. Liebling, Orbital dy- namics of binary boson star systems, Phys. Rev. D77, 044036 (2008)

  39. [39]

    Sanchis-Gual, J

    N. Sanchis-Gual, J. C. Bustillo, C. Herdeiro, E. Radu, J. A. Font, S. H. W. Leong, and A. Torres-Forn´ e, Im- pact of the wavelike nature of proca stars on their gravitational-wave emission, Phys. Rev. D106, 124011 (2022)

  40. [40]

    Croft, T

    R. Croft, T. Helfer, B.-X. Ge, M. Radia, T. Evstafyeva, 17 E. A. Lim, U. Sperhake, and K. Clough, The gravita- tional afterglow of boson stars, Classical and Quantum Gravity40, 065001 (2023)

  41. [41]

    B.-X. Ge, E. A. Lim, U. Sperhake, T. Evstafyeva, D. Cors, E. de Jong, R. Croft, and T. Helfer, Dynamics and gravitational radiation of stable and unstable boson- star mergers, Physical Review D112, 124080 (2025)

  42. [42]

    Palenzuela, P

    C. Palenzuela, P. Pani, M. Bezares, V. Cardoso, L. Lehner, and S. Liebling, Gravitational wave signatures of highly compact boson star binaries, Phys. Rev. D96, 104058 (2017)

  43. [43]

    Bezares, C

    M. Bezares, C. Palenzuela, and C. Bona, Final fate of compact boson star mergers, Physical Review D95, 124005 (2017)

  44. [44]

    Palenzuela, P

    C. Palenzuela, P. Pani, M. Bezares, V. Cardoso, L. Lehner, and S. Liebling, Gravitational wave signatures of highly compact boson star binaries, Physical Review D96, 104058 (2017)

  45. [45]

    Bezares, M

    M. Bezares, M. Boˇ skovi´ c, S. Liebling, C. Palenzuela, P. Pani, and E. Barausse, Gravitational waves and kicks from the merger of unequal mass, highly compact boson stars, Physical Review D105, 064067 (2022)

  46. [46]

    Evstafyeva, U

    T. Evstafyeva, U. Sperhake, I. M. Romero-Shaw, and M. Agathos, Gravitational-wave data analysis with high- precision numerical relativity simulations of boson star mergers, Physical Review Letters133, 131401 (2024)

  47. [47]

    Lessons from binary dynamics of inspiralling equal-mass boson-star mergers

    T. Evstafyeva, A. Seifert, U. Sperhake, C. J. Moore, and T. Jain, Lessons from binary dynamics of inspiralling equal-mass boson-star mergers (2026), arXiv:2604.25582 [gr-qc]

  48. [48]

    Sanchis-Gual, M

    N. Sanchis-Gual, M. Zilh˜ ao, C. Herdeiro, F. Di Gio- vanni, J. A. Font, and E. Radu, Synchronized gravita- tional atoms from mergers of bosonic stars, Physical Re- view D102, 101504 (2020)

  49. [49]

    Palloni, N

    G. Palloni, N. Sanchis-Gual, J. A. Font, C. Herdeiro, and E. Radu, Eccentric mergers of binary proca stars, Phys. Rev. D112, 104011 (2025)

  50. [50]

    Bezares and C

    M. Bezares and C. Palenzuela, Gravitational waves from dark boson star binary mergers, Classical and Quantum Gravity35, 234002 (2018)

  51. [51]

    Sanchis-Gual, C

    N. Sanchis-Gual, C. Herdeiro, J. A. Font, E. Radu, and F. Di Giovanni, Head-on collisions and orbital mergers of proca stars, Phys. Rev. D99, 024017 (2019)

  52. [52]

    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)

  53. [53]

    Croft, T

    R. Croft, T. Helfer, B.-X. Ge, M. Radia, T. Evstafyeva, E. A. Lim, U. Sperhake, and K. Clough, The gravita- tional afterglow of boson stars, Classical and Quantum Gravity40, 065001 (2023)

  54. [54]

    Helfer, E

    T. Helfer, E. A. Lim, M. A. G. Garcia, and M. A. Amin, Gravitational wave emission from collisions of compact scalar solitons, Phys. Rev. D99, 044046 (2019)

  55. [55]

    Helfer, U

    T. Helfer, U. Sperhake, R. Croft, M. Radia, B.-X. Ge, and E. A. Lim, Malaise and remedy of binary boson-star initial data, Classical and Quantum Gravity39, 074001 (2022)

  56. [56]

    Evstafyeva, U

    T. Evstafyeva, U. Sperhake, T. Helfer, R. Croft, M. Ra- dia, B.-X. Ge, and E. A. Lim, Unequal-mass boson-star binaries: initial data and merger dynamics, Classical and Quantum Gravity40, 085009 (2023)

  57. [57]

    Atteneder, H

    F. Atteneder, H. R. R¨ uter, D. Cors, R. Rosca-Mead, D. Hilditch, and B. Br¨ ugmann, Boson star head-on colli- sions with constraint-violating and constraint-satisfying initial data, Phys. Rev. D109, 044058 (2024)

  58. [58]

    J. C. Aurrekoetxea, K. Clough, and E. A. Lim, Cttk: a new method to solve the initial data constraints in nu- merical relativity, Classical and Quantum Gravity40, 075003 (2023)

  59. [59]

    Siemonsen and W

    N. Siemonsen and W. E. East, Binary boson stars: Merger dynamics and formation of rotating remnant stars, Phys. Rev. D107, 124018 (2023)

  60. [60]

    Siemonsen and W

    N. Siemonsen and W. E. East, Generic initial data for binary boson stars, Phys. Rev. D108, 124015 (2023)

  61. [61]

    J. C. Aurrekoetxea, S. E. Brady, L. Arest´ e-Sal´ o, J. Bam- ber, L. Chung-Jukko, K. Clough, E. de Jong, M. Elley, P. Figueras, T. Helfer, E. A. Lim, M. Radia, A. Waem- ing, and Z. Wang, Grtresna: An open-source code to solve the initial data constraints in numerical relativity (2025), arXiv:2501.13046 [gr-qc]

  62. [62]

    H. P. PFEIFFER, The initial value prob- lem in numerical relativity, Journal of Hyper- bolic Differential Equations02, 497 (2005), https://doi.org/10.1142/S0219891605000518

  63. [63]

    H. P. Pfeiffer and J. W. York, Uniqueness and nonunique- ness in the einstein constraints, Phys. Rev. Lett.95, 091101 (2005)

  64. [64]

    T. W. Baumgarte, N. O. Murchadha, and H. P. Pfeiffer, Einstein constraints: Uniqueness and nonuniqueness in the conformal thin sandwich approach, Phys. Rev. D75, 044009 (2007)

  65. [65]

    Cordero-Carri´ on, P

    I. Cordero-Carri´ on, P. Cerd´ a-Dur´ an, H. Dimmelmeier, J. L. Jaramillo, J. Novak, and E. Gourgoulhon, Improved constrained scheme for the einstein equations: An ap- proach to the uniqueness issue, Phys. Rev. D79, 024017 (2009)

  66. [66]

    J. R. Wilson, G. J. Mathews, and P. Marronetti, Rela- tivistic numerical model for close neutron-star binaries, Phys. Rev. D54, 1317 (1996)

  67. [67]

    J. A. ISENBERG, Waveless approxima- tion theories of gravity, International Jour- nal of Modern Physics D17, 265 (2008), https://doi.org/10.1142/S0218271808011997

  68. [68]

    Bonazzola, E

    S. Bonazzola, E. Gourgoulhon, P. Grandcl´ ement, and J. Novak, Constrained scheme for the einstein equations based on the dirac gauge and spherical coordinates, Phys. Rev. D70, 104007 (2004)

  69. [69]

    Cordero-Carri´ on, J

    I. Cordero-Carri´ on, J. M. Ib´ a˜ nez, E. Gourgoulhon, J. L. Jaramillo, and J. Novak, Mathematical issues in a fully constrained formulation of the einstein equations, Phys. Rev. D77, 084007 (2008)

  70. [70]

    Rinne, Constrained evolution in axisymmetry and the gravitational collapse of prolate brill waves, Classical and Quantum Gravity25, 135009 (2008)

    O. Rinne, Constrained evolution in axisymmetry and the gravitational collapse of prolate brill waves, Classical and Quantum Gravity25, 135009 (2008)

  71. [71]

    Taylor,Partial differential equations: Nonlinear equa- tions, Applied mathematical sciences No

    M. Taylor,Partial differential equations: Nonlinear equa- tions, Applied mathematical sciences No. v. 3 (Springer, 1996)

  72. [72]

    Protter and H

    M. Protter and H. Weinberger,Maximum Principles in Differential Equations, Prentice-Hall partial differential equations series (Prentice-Hall, 1967)

  73. [73]

    Evans,Partial Differential Equations, Graduate stud- ies in mathematics (American Mathematical Society, 1998)

    L. Evans,Partial Differential Equations, Graduate stud- ies in mathematics (American Mathematical Society, 1998)

  74. [74]

    Di Giovanni, N

    F. Di Giovanni, N. Sanchis-Gual, D. Guerra, M. Miravet- Ten´ es, P. Cerd´ a-Dur´ an, and J. A. Font, Impact of ultra- light bosonic dark matter on the dynamical bar-mode instability of rotating neutron stars, Phys. Rev. D106, 18 044008 (2022), arXiv:2206.00977 [gr-qc]

  75. [75]

    Adsuara, I

    J. Adsuara, I. Cordero-Carri´ on, P. Cerd´ a-Dur´ an, and M. Aloy, Scheduled relaxation jacobi method: Im- provements and applications, Journal of Computational Physics321, 369 (2016)

  76. [76]

    Adsuara, I

    J. Adsuara, I. Cordero-Carri´ on, P. Cerd´ a-Dur´ an, V. Mewes, and M. Aloy, On the equivalence between the scheduled relaxation jacobi method and richardson’s non- stationary method, Journal of Computational Physics 332, 446 (2017)

  77. [77]

    Banchelli, M

    F. Banchelli, M. Garcia-Gasulla, F. Mantovani, J. Vinyals, J. Pocurull, D. Vicente, B. Eguzkitza, F. C. C. Galeazzo, M. C. Acosta, and S. Girona, Introducing marenostrum5: A european pre-exascale energy-efficient system designed to serve a broad spectrum of scientific workloads (2025), arXiv:2503.09917 [cs.DC]

  78. [78]

    Santos-P´ erez, I

    S. Santos-P´ erez, I. Cordero-Carri´ on, and P. Cerd´ a- Dur´ an, Reformulation of einstein equations in the fully constrained formulation: Local-uniqueness, post- newtonian expansion, and initial data, Phys. Rev. D112, 024057 (2025)

  79. [79]

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

  80. [80]

    C. Lazarte, Estrellas deℓ-Proca: generalizaci´ on mul- ticampo en simetr´ ıa esf´ erica de estrellas de Proca con momento angular, Master’s thesis, Universidad Nacional Aut´ onoma de M´ exico (2023)

Showing first 80 references.