pith. machine review for the scientific record. sign in

arxiv: 2604.02412 · v1 · submitted 2026-04-02 · 🌌 astro-ph.GA · astro-ph.SR

Recognition: 2 theorem links

· Lean Theorem

An analytical approach to binary populations in globular clusters

Authors on Pith no claims yet

Pith reviewed 2026-05-13 20:53 UTC · model grok-4.3

classification 🌌 astro-ph.GA astro-ph.SR
keywords globular clustersbinary fractionsdynamical evolutionprimordial binarieshard soft boundarystellar black holes
0
0 comments X

The pith

Dynamical dissolution of soft primordial binaries fully explains the low main-sequence binary fractions in present-day globular clusters.

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

The paper shows that globular clusters display lower binary fractions than field stars because soft primordial binaries are disrupted by dynamical encounters over the cluster lifetime. Assuming the initial binary distribution matches that in the solar neighborhood, simple analytical estimates of the hard-soft boundary and binary ionization rates reproduce the observed fractions without requiring different star formation physics at low metallicity or high density. These estimates are checked against a full Cluster Monte Carlo N-body simulation and remain consistent. The argument further implies that the present binary fraction in any cluster encodes its birth radius, pointing to similar formation conditions for surviving Milky Way globular clusters and local young massive clusters. Stellar black holes are identified as essential because their burning sustains the dynamical heating that continues to process the binary population.

Core claim

Starting from the assumption that the initial binary distribution in GCs is the same as the binary distribution observed in the solar neighborhood, the dynamical dissolution of soft primordial binaries can fully explain the main-sequence binary fractions in present-day GCs. This is validated against a detailed N-body simulation with the Cluster Monte Carlo code. Adopting the view that the observed binary fraction in a given cluster constrains the location of the hard/soft boundary at birth, surviving Milky Way GCs had a similar distribution of birth radii to young massive clusters in the local universe. Stellar black holes play a crucial role through black hole burning in sculpting GC binary

What carries the argument

The hard/soft boundary for binary orbits, defined by the point where a binary's binding energy equals the average kinetic energy of field stars; soft binaries are ionized by encounters while hard binaries survive and harden.

If this is right

  • The observed binary fraction directly constrains the birth radius of each globular cluster through the location of the hard/soft boundary.
  • Stellar black holes are required to sustain the dynamical heating that continues to ionize soft binaries throughout the cluster lifetime.
  • Realistic initial conditions that include both a solar-neighborhood-like binary population and a full stellar black hole population are necessary for any dynamical model of globular clusters.
  • Milky Way globular clusters that survive to the present day formed with radii comparable to those of young massive clusters observed in the local universe.

Where Pith is reading between the lines

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

  • If the mechanism holds, binary fractions measured in globular clusters of different dynamical ages should follow a simple scaling with the number of relaxation times experienced since birth.
  • The same analytical framework could be applied to open clusters or nuclear star clusters to predict how their binary populations evolve under weaker tidal fields.
  • Metallicity dependence would enter only indirectly through the black-hole mass spectrum rather than through any change in the primordial binary fraction itself.

Load-bearing premise

The initial binary fraction and orbital distribution in globular clusters at formation matched the distribution observed among main-sequence stars in the solar neighborhood.

What would settle it

Direct measurement of binary fractions and period distributions in a statistically large sample of young massive clusters that would show initial soft-binary fractions significantly lower than those assumed for the solar neighborhood.

Figures

Figures reproduced from arXiv: 2604.02412 by Christopher E. O'Connor, Frederic A. Rasio, Kyle Kremer.

Figure 1
Figure 1. Figure 1: Map of the primary mass–semimajor axis param￾eter space for binary systems embedded in fiducial Plummer– sphere clusters. Solid lines show the hard/soft boundary as a function of m1 in each cluster for binaries with mass ratio q = 0.5; the color of each line indicates the cluster param￾eters described in the text: blue for model A, amber for B, green for C, and red for D. Dashed lines of the correspond￾ing… view at source ↗
Figure 2
Figure 2. Figure 2: Binary fraction as a function of primary mass. The black points are the measured MF among MS stars in the solar neighborhood as compiled in [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Like [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Key timescales related to soft binary evolution within GCs, as computed for fiducial models A through D. The background stars assumed to have an average mass of ¯m = 0.6M⊙ and a binary fraction of Fb = 0.3. Colored curves show the strong encounter interval as a function of η for soft binaries of various masses. The black horizontal lines indicate the cluster’s half-mass crossing time Tcross, the mass segre… view at source ↗
Figure 5
Figure 5. Figure 5: Results of a CMC simulation of a GC with a primordial binary population realized according to our fiducial IBD. Clockwise from the top left, the four panels show (i) the total number of bound stars (blue) and total bound mass (amber), normalized to their initial values; (ii) the half-mass radius (blue) and theoretical (density-weighted) core radius (amber); (iii) the number of bound BHs (blue) and binary B… view at source ↗
Figure 6
Figure 6. Figure 6: Observed binary fraction versus cluster radius for a sample of 29 well-studied Milky Way GCs (J. Ji & J. N. Bregman 2015; H. Baumgardt & M. Hilker 2018). Small points show the observed half-mass radius of each cluster, while large points and vertical error bars indicate the range of plausible virial radii implied by our analytical model. The coloration of each point corresponds to the cluster’s nominal bir… view at source ↗
read the original abstract

Globular clusters (GCs) display much lower binary fractions than found among main-sequence stars in the solar neighborhood. The physical cause of this difference is debatable: does it reflect different star formation outcomes at low metallicity and/or high density, the dynamical processing of primordial binaries over cluster lifetimes, or a combination of the two? Starting from the assumption that the initial binary distribution in GCs is the same as the binary distribution observed in the solar neighborhood, we show with straightforward analytical calculations that the dynamical dissolution of "soft" primordial binaries can fully explain the main-sequence binary fractions in present-day GCs. We validate our estimates against a detailed N-body simulation with the Cluster Monte Carlo code. Adopting the view that the observed binary fraction in a given cluster constrains the location of the hard/soft boundary at birth, we infer that surviving Milky Way GCs had a similar distribution of birth radii to young massive clusters in the local universe. Our findings underscore the crucial role of stellar black holes (through "black hole burning") in sculpting GC binary populations and reinforce the need for realistic initial conditions in theoretical modeling of GC dynamics.

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 claims that, starting from the assumption that the initial binary distribution in globular clusters matches the solar-neighborhood field population, straightforward analytical calculations of the dynamical ionization of soft primordial binaries over a Hubble time can fully explain the observed main-sequence binary fractions (0.05–0.2) in present-day GCs. The estimates are validated against Cluster Monte Carlo N-body simulations; the observed fractions are then used to constrain the hard/soft boundary location at birth and infer that surviving Milky Way GCs had birth radii similar to local young massive clusters, with stellar black holes playing a key role via black-hole burning.

Significance. If the stated initial-condition assumption holds, the work supplies a transparent, low-parameter analytical framework that reproduces simulation results and isolates the dynamical contribution to binary depletion, reinforcing the importance of realistic initial conditions and black-hole dynamics in GC modeling. The approach offers a clear falsifiable pathway (via future constraints on primordial binary distributions at low metallicity) and complements full N-body studies without replacing them.

minor comments (2)
  1. [Abstract] Abstract: the phrasing 'can fully explain' is accurate only under the explicit premise of identical initial distributions; a parenthetical reminder of this condition would prevent misreading as an unconditional result.
  2. [Conclusions] The manuscript should add a short sensitivity discussion (perhaps in the conclusions) on how the inferred birth-radius distribution would shift if GC formation suppressed the soft-binary tail relative to the solar-neighborhood distribution, even if the central derivation remains unchanged.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive assessment of our work and the recommendation for minor revision. The review correctly identifies the core claim that dynamical ionization of soft primordial binaries, under solar-neighborhood initial conditions, can account for the observed main-sequence binary fractions in present-day globular clusters. We will incorporate the minor changes suggested.

Circularity Check

0 steps flagged

Derivation independent; explicit assumption plus external simulation check

full rationale

The paper states upfront the assumption that initial GC binary distributions match the solar-neighborhood field population, then applies standard hard/soft ionization criteria to compute the surviving fraction after a Hubble time. This produces the observed GC binary fractions (0.05-0.2) from an assumed starting value (~0.5) without redefining the target quantity in terms of itself. The analytical result is cross-validated against CMC N-body runs that use the same initial conditions but are an independent numerical realization. No equation reduces the final binary fraction to a fitted parameter or to a self-citation chain; the hard/soft boundary location is taken as an observable constraint rather than adjusted to force agreement. The single minor self-citation (likely to prior CMC methodology) is not load-bearing for the central analytical claim.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on one domain assumption about initial conditions and treats the hard/soft boundary location as a parameter constrained by observed binary fractions to infer birth radii.

free parameters (1)
  • hard/soft boundary location at birth
    Constrained by the observed binary fraction in each cluster to infer birth radii; not a free fit but an inference step.
axioms (1)
  • domain assumption Initial binary distribution in GCs is identical to the solar-neighborhood distribution
    Explicit starting assumption stated in the abstract that enables the analytical calculation.

pith-pipeline@v0.9.0 · 5498 in / 1196 out tokens · 38476 ms · 2026-05-13T20:53:35.850670+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.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Black Hole Binary Detection Landscape for the Laser Interferometer Lunar Antenna (LILA): Signal-to-Noise Calculations & Science Cases

    astro-ph.HE 2026-05 unverdicted novelty 5.0

    LILA can detect IMBH binaries at redshifts 20-30, IMRIs, and provide months-to-years early warnings with high-SNR events for gravity tests.

Reference graph

Works this paper leans on

102 extracted references · 102 canonical work pages · cited by 1 Pith paper · 2 internal anchors

  1. [1]

    P., Abbott, R., Abbott, T

    Abbott, B. P., Abbott, R., Abbott, T. D., et al. 2016, PhRvD, 93, 122003, doi: 10.1103/PhysRevD.93.122003

  2. [2]

    The Astrophysical Journal , author =

    Albrow, M. D., Gilliland, R. L., Brown, T. M., et al. 2001, ApJ, 559, 1060, doi: 10.1086/322353

  3. [3]

    2018, MNRAS, 478, 1844, doi: 10.1093/mnras/sty1186

    Askar, A., Arca Sedda, M., & Giersz, M. 2018, MNRAS, 478, 1844, doi: 10.1093/mnras/sty1186

  4. [4]

    C., Trani, A

    Atallah, D., Weatherford, N. C., Trani, A. A., & Rasio, F. A. 2024, ApJ, 970, 112, doi: 10.3847/1538-4357/ad5185

  5. [5]

    2010, ApJ, 708, 834, doi: 10.1088/0004-637X/708/1/834

    Bartko, H., Martins, F., Trippe, S., et al. 2010, ApJ, 708, 834, doi: 10.1088/0004-637X/708/1/834

  6. [6]

    2025, MNRAS, 541, 2008, doi: 10.1093/mnras/staf1102

    Bashi, D., & Belokurov, V. 2025, MNRAS, 541, 2008, doi: 10.1093/mnras/staf1102

  7. [7]

    A., & de Grijs, R

    Scheepmaker, R. A., & de Grijs, R. 2005, A&A, 431, 905, doi: 10.1051/0004-6361:20041078

  8. [8]

    Monthly Notices of the Royal Astronomical Society , author =

    Baumgardt, H., & Hilker, M. 2018, MNRAS, 478, 1520, doi: 10.1093/mnras/sty1057

  9. [9]

    Rocha-Pinto, H. J. 2017, MNRAS, 471, 2812, doi: 10.1093/mnras/stx1763

  10. [10]

    G., & Heggie, D

    Breen, P. G., & Heggie, D. C. 2013, MNRAS, 432, 2779, doi: 10.1093/mnras/stt628

  11. [11]

    2020 , note =

    Breivik, K., Coughlin, S., Zevin, M., et al. 2020, ApJ, 898, 71, doi: 10.3847/1538-4357/ab9d85

  12. [12]

    Galactic

    Chabrier, G. 2003, PASP, 115, 763, doi: 10.1086/376392

  13. [13]

    M., & Rasio, F

    Chatterjee, S., Umbreit, S., Fregeau, J. M., & Rasio, F. A. 2013, MNRAS, 429, 2881, doi: 10.1093/mnras/sts464

  14. [14]

    C., Geller, A

    Childs, A. C., Geller, A. M., von Hippel, T., Motherway, E., & Zwicker, C. 2024, ApJ, 962, 41, doi: 10.3847/1538-4357/ad18c0

  15. [15]

    J., et al

    Chomiuk, L., Strader, J., Maccarone, T. J., et al. 2013, ApJ, 777, 69, doi: 10.1088/0004-637X/777/1/69

  16. [16]

    S., Do, T., Ghez, A., et al

    Chu, D. S., Do, T., Ghez, A., et al. 2023, ApJ, 948, 94, doi: 10.3847/1538-4357/acc93e

  17. [17]

    Ritchie, B. W. 2023, MNRAS, 521, 4473, doi: 10.1093/mnras/stad449

  18. [18]

    S., Ritchie, B

    Clark, J. S., Ritchie, B. W., & Negueruela, I. 2020, A&A, 635, A187, doi: 10.1051/0004-6361/201935903

  19. [19]

    I., Girard, T

    Dinescu, D. I., Girard, T. M., & van Altena, W. F. 1999, AJ, 117, 1792, doi: 10.1086/300807

  20. [20]

    1991, A&A, 248, 485

    Duquennoy, A., & Mayor, M. 1991, A&A, 248, 485

  21. [21]

    2019, MNRAS, 482, L139, doi: 10.1093/mnrasl/sly206

    El-Badry, K., & Rix, H.-W. 2019, MNRAS, 482, L139, doi: 10.1093/mnrasl/sly206

  22. [22]

    C., Pringle, J

    Fabian, A. C., Pringle, J. E., & Rees, M. J. 1975, MNRAS, 172, 15, doi: 10.1093/mnras/172.1.15P

  23. [23]

    M., Ivanova, N., & Rasio, F

    Fregeau, J. M., Ivanova, N., & Rasio, F. A. 2009, ApJ, 707, 1533, doi: 10.1088/0004-637X/707/2/1533

  24. [24]

    M., & Rasio, F

    Fregeau, J. M., & Rasio, F. A. 2007, ApJ, 658, 1047, doi: 10.1086/511809

  25. [25]

    2021, ApJ, 922, 110, doi: 10.3847/1538-4357/ac2610

    Kalogera, V. 2021, ApJ, 922, 110, doi: 10.3847/1538-4357/ac2610

  26. [26]

    K., Do, T., Ghez, A

    Gautam, A. K., Do, T., Ghez, A. M., et al. 2024, ApJ, 964, 164, doi: 10.3847/1538-4357/ad26e6

  27. [27]

    M., de Grijs, R., Li, C., & Hurley, J

    Geller, A. M., de Grijs, R., Li, C., & Hurley, J. R. 2013, ApJ, 779, 30, doi: 10.1088/0004-637X/779/1/30

  28. [28]

    2025, arXiv e-prints, arXiv:2510.06942, doi: 10.48550/arXiv.2510.06942 Gonz´ alez Prieto, E., Kremer, K., Chatterjee, S., et al

    Giersz, M., Askar, A., Hypki, A., et al. 2025, arXiv e-prints, arXiv:2510.06942, doi: 10.48550/arXiv.2510.06942 Gonz´ alez Prieto, E., Kremer, K., Chatterjee, S., et al. 2021, ApJL, 908, L29, doi: 10.3847/2041-8213/abdf5b 16O’Connor, Kremer & Rasio Gonz´ alez Prieto, E., Kremer, K., Fragione, G., et al. 2022, ApJ, 940, 131, doi: 10.3847/1538-4357/ac9b0f G...

  29. [29]

    Kremer, K., & Rasio, F. A. 2024, ApJ, 969, 29, doi: 10.3847/1538-4357/ad43d6

  30. [30]

    1984, ApJ, 280, 298, doi: 10.1086/161996 Grudi´ c, M

    Goodman, J. 1984, ApJ, 280, 298, doi: 10.1086/161996 Grudi´ c, M. Y., Guszejnov, D., Hopkins, P. F., Offner, S. S. R., & Faucher-Gigu` ere, C.-A. 2021, MNRAS, 506, 2199, doi: 10.1093/mnras/stab1347

  31. [31]

    Guszejnov, D., Markey, C., Offner, S. S. R., et al. 2022, MNRAS, 515, 167, doi: 10.1093/mnras/stac1737

  32. [32]

    N., Offner, S

    Guszejnov, D., Raju, A. N., Offner, S. S. R., et al. 2023, MNRAS, 518, 4693, doi: 10.1093/mnras/stac3268

  33. [33]

    R., Millman, K

    Harris, C. R., Millman, K. J., van der Walt, S. J., et al. 2020, Nature, 585, 357, doi: 10.1038/s41586-020-2649-2

  34. [34]

    2003, The Gravitational Million-Body Problem: A Multidisciplinary Approach to Star Cluster Dynamics

    Heggie, D., & Hut, P. 2003, The Gravitational Million-Body Problem: A Multidisciplinary Approach to Star Cluster Dynamics

  35. [35]

    Heggie, D. C. 1975, MNRAS, 173, 729, doi: 10.1093/mnras/173.3.729 H´ enon, M. 1971a, Ap&SS, 13, 284, doi: 10.1007/BF00649159 H´ enon, M. 1971b, Ap&SS, 14, 151, doi: 10.1007/BF00649201

  36. [36]

    2020, MNRAS, 498, 3,

    Hong, J., Vesperini, E., Askar, A., et al. 2018, MNRAS, 480, 5645, doi: 10.1093/mnras/sty2211

  37. [37]

    2017, MNRAS, 464, 2511, doi: 10.1093/mnras/stw2595

    Hong, J., Vesperini, E., Belloni, D., & Giersz, M. 2017, MNRAS, 464, 2511, doi: 10.1093/mnras/stw2595

  38. [38]

    2015, MNRAS, 449, 629, doi: 10.1093/mnras/stv306

    Hong, J., Vesperini, E., Sollima, A., et al. 2015, MNRAS, 449, 629, doi: 10.1093/mnras/stv306

  39. [39]

    W., Lu, J

    Hosek, Jr., M. W., Lu, J. R., Anderson, J., et al. 2019, ApJ, 870, 44, doi: 10.3847/1538-4357/aaef90

  40. [40]

    Hunter, J. D. 2007, Computing in Science and Engineering, 9, 90, doi: 10.1109/MCSE.2007.55

  41. [41]

    R., Aarseth, S

    Hurley, J. R., Aarseth, S. J., & Shara, M. M. 2007, ApJ, 665, 707, doi: 10.1086/517879

  42. [42]

    Hut, P., McMillan, S., & Romani, R. W. 1992a, ApJ, 389, 527, doi: 10.1086/171229

  43. [43]

    1992b, PASP, 104, 981, doi: 10.1086/133085

    Hut, P., McMillan, S., Goodman, J., et al. 1992b, PASP, 104, 981, doi: 10.1086/133085

  44. [44]

    C., Zakamska, N

    Hwang, H.-C., Ting, Y.-S., Schlaufman, K. C., Zakamska, N. L., & Wyse, R. F. G. 2021, MNRAS, 501, 4329, doi: 10.1093/mnras/staa3854

  45. [45]

    2025, A&A, 693, A41, doi: 10.1051/0004-6361/202348653

    Hypki, A., Vesperini, E., Giersz, M., et al. 2025, A&A, 693, A41, doi: 10.1051/0004-6361/202348653

  46. [46]

    A., Brink, T

    Irwin, J. A., Brink, T. G., Bregman, J. N., & Roberts, T. P. 2010, ApJL, 712, L1, doi: 10.1088/2041-8205/712/1/L1

  47. [47]

    2005 , month = sep, journal =

    Ivanova, N., Belczynski, K., Fregeau, J. M., & Rasio, F. A. 2005, MNRAS, 358, 572, doi: 10.1111/j.1365-2966.2005.08804.x

  48. [48]

    Fregeau, J. M. 2008, MNRAS, 386, 553, doi: 10.1111/j.1365-2966.2008.13064.x Jeˇ r´ abkov´ a, T., Kroupa, P., Dabringhausen, J., Hilker, M., & Bekki, K. 2017, A&A, 608, A53, doi: 10.1051/0004-6361/201731240

  49. [49]

    Ji, J., & Bregman, J. N. 2015, ApJ, 807, 32, doi: 10.1088/0004-637X/807/1/32

  50. [50]

    J., Rasio, F

    Joshi, K. J., Rasio, F. A., & Portegies Zwart, S. 2000, ApJ, 540, 969, doi: 10.1086/309350

  51. [51]

    Kamlah, A. W. H., Leveque, A., Spurzem, R., et al. 2022, MNRAS, 511, 4060, doi: 10.1093/mnras/stab3748

  52. [52]

    The Astronomical Journal , author =

    King, I. 1962, AJ, 67, 471, doi: 10.1086/108756 Kıro˘ glu, F., Kremer, K., & Rasio, F. A. 2025, ApJL, 994, L37, doi: 10.3847/2041-8213/ae1eeb

  53. [53]

    2026, in Encyclopedia of Astrophysics, Volume 3, Vol

    Kremer, K. 2026, in Encyclopedia of Astrophysics, Volume 3, Vol. 3, 458–472, doi: 10.1016/B978-0-443-21439-4.00103-6

  54. [54]

    L., & Rasio, F

    Kremer, K., Chatterjee, S., Rodriguez, C. L., & Rasio, F. A. 2018, ApJ, 852, 29, doi: 10.3847/1538-4357/aa99df

  55. [55]

    Rasio, F. A. 2019, ApJ, 871, 38, doi: 10.3847/1538-4357/aaf646

  56. [56]

    L., & Li, D

    Kremer, K., Piro, A. L., & Li, D. 2021, ApJL, 917, L11, doi: 10.3847/2041-8213/ac13a0

  57. [57]

    C., Hopkins, P

    Kremer, K., Weatherford, N. C., Hopkins, P. F., Rui, N. Z., & Ye, C. S. 2025, ApJL, 993, L34, doi: 10.3847/2041-8213/ae1233

  58. [58]

    S., Rui, N

    Kremer, K., Ye, C. S., Rui, N. Z., et al. 2020, ApJS, 247, 48, doi: 10.3847/1538-4365/ab7919

  59. [59]

    1995, MNRAS, 277, 1507, doi: 10.1093/mnras/277.4.1507

    Kroupa, P. 1995, MNRAS, 277, 1507, doi: 10.1093/mnras/277.4.1507

  60. [60]

    2001, MNRAS, 322, 231, doi: 10.1046/j.1365-8711.2001.04022.x

    Kroupa, P. 2001, MNRAS, 322, 231, doi: 10.1046/j.1365-8711.2001.04022.x

  61. [61]

    R., McKee, C

    Krumholz, M. R., McKee, C. F., & Bland-Hawthorn, J. 2019, ARA&A, 57, 227, doi: 10.1146/annurev-astro-091918-104430

  62. [62]

    Leigh, N. W. C., Giersz, M., Marks, M., et al. 2015, MNRAS, 446, 226, doi: 10.1093/mnras/stu2110

  63. [63]

    Leigh, N. W. C., Giersz, M., Webb, J. J., et al. 2013, MNRAS, 436, 3399, doi: 10.1093/mnras/stt1825

  64. [64]

    2025, ApJL, 982, L43, doi: 10.3847/2041-8213/adbe60

    Liu, R., Shao, Z., & Li, L. 2025, ApJL, 982, L43, doi: 10.3847/2041-8213/adbe60

  65. [65]

    R., Do, T., Ghez, A

    Lu, J. R., Do, T., Ghez, A. M., et al. 2013, ApJ, 764, 155, doi: 10.1088/0004-637X/764/2/155

  66. [66]

    J., Kundu, A., Zepf, S

    Maccarone, T. J., Kundu, A., Zepf, S. E., & Rhode, K. L. 2007, Nature, 445, 183, doi: 10.1038/nature05434

  67. [67]

    D., Wilkinson, M

    Mackey, A. D., Wilkinson, M. I., Davies, M. B., & Gilmore, G. F. 2007, MNRAS, 379, L40, doi: 10.1111/j.1745-3933.2007.00330.x Binaries in globular clusters17

  68. [68]

    and Wilkinson, M

    Mackey, A. D., Wilkinson, M. I., Davies, M. B., & Gilmore, G. F. 2008, MNRAS, 386, 65, doi: 10.1111/j.1365-2966.2008.13052.x

  69. [69]

    Martinez, M. A. S., Fragione, G., Kremer, K., et al. 2020, ApJ, 903, 67, doi: 10.3847/1538-4357/abba25

  70. [70]

    Matzner, C. D. 2024, ApJL, 975, L17, doi: 10.3847/2041-8213/ad85d4

  71. [71]

    McMillan, S. L. W., McDermott, P. N., & Taam, R. E. 1987, ApJ, 318, 261, doi: 10.1086/165365

  72. [72]

    P., Piotto, G., Bedin, L

    Milone, A. P., Piotto, G., Bedin, L. R., et al. 2012, A&A, 540, A16, doi: 10.1051/0004-6361/201016384

  73. [73]
  74. [74]

    M., & Badenes, C

    Moe, M., Kratter, K. M., & Badenes, C. 2019, ApJ, 875, 61, doi: 10.3847/1538-4357/ab0d88

  75. [75]

    A., & Umbreit, S

    Morscher, M., Pattabiraman, B., Rodriguez, C., Rasio, F. A., & Umbreit, S. 2015, ApJ, 800, 9, doi: 10.1088/0004-637X/800/1/9

  76. [76]

    M., & Rasio, F

    Morscher, M., Umbreit, S., Farr, W. M., & Rasio, F. A. 2013, ApJL, 763, L15, doi: 10.1088/2041-8205/763/1/L15 M¨ uller-Horn, J., G¨ ottgens, F., Dreizler, S., et al. 2025, A&A, 693, A161, doi: 10.1051/0004-6361/202450709

  77. [77]

    Offner, S. S. R., Moe, M., Kratter, K. M., et al. 2023, in Astronomical Society of the Pacific Conference Series, Vol. 534, Protostars and Planets VII, ed. S. Inutsuka, Y. Aikawa, T. Muto, K. Tomida, & M. Tamura, 275, doi: 10.48550/arXiv.2203.10066

  78. [78]

    2025, ApJL, 994, L54, doi: 10.3847/2041-8213/ae1447

    Sedda, M. 2025, ApJL, 994, L54, doi: 10.3847/2041-8213/ae1447

  79. [79]

    2013, ApJS, 204, 15, doi: 10.1088/0067-0049/204/2/15

    Pattabiraman, B., Umbreit, S., Liao, W.-k., et al. 2013, ApJS, 204, 15, doi: 10.1088/0067-0049/204/2/15

  80. [80]

    2026, arXiv e-prints, arXiv:2603.06790, doi: 10.48550/arXiv.2603.06790 Portegies Zwart, S

    Phillips, A., Conroy, C., Nibauer, J., et al. 2026, arXiv e-prints, arXiv:2603.06790, doi: 10.48550/arXiv.2603.06790 Portegies Zwart, S. F., McMillan, S. L. W., & Gieles, M. 2010, ARA&A, 48, 431, doi: 10.1146/annurev-astro-081309-130834

Showing first 80 references.