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  • Open Access

Analytical, Statistical Approximate Solution of Dissipative and Nondissipative Binary-Single Stellar Encounters

Yonadav Barry Ginat* and Hagai B. Perets†

  • Faculty of Physics, Technion-Israel Institute of Technology, Haifa, 3200003, Israel

  • *ginat@campus.technion.ac.il
  • †hperets@physics.technion.ac.il

Phys. Rev. X 11, 031020 – Published 23 July, 2021

DOI: https://doi.org/10.1103/PhysRevX.11.031020

Abstract

We present a statistical approximate solution of the bound, nonhierarchical three-body problem, and extend it to a general analysis of encounters between hard binary systems and single stars. Any such encounter terminates when one of the three stars is ejected to infinity, leaving behind a remnant binary; the problem with binary-single-star scattering consists of finding the probability distribution of the orbital parameters of the remnant binary as a function of the total energy and the total angular momentum. Here, we model the encounter as a series of close, nonhierarchical, triple approaches, interspersed with hierarchical phases, in which the system consists of an inner binary and a star that orbits it; this series of approaches turns the evolution of the entire encounter to a random walk between consecutive hierarchical phases. We use the solution of the bound, nonhierarchical three-body problem to find the walker’s transition probabilities, which we generalize to situations in which tidal interactions are important. Besides tides, any dissipative process may be incorporated into the random-walk model, as it is completely general. Our approximate solution can reproduce the results of the extensive body of past numerical simulations and can account for different environments and different dissipative effects. Therefore, this model can effectively replace the need for direct few-body integrations for the study of binary-single encounters in any environment. Furthermore, it allows for a simply inclusion of dissipative forces typically not accounted for in full N-body integration schemes.

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Corrections

28 April, 2022

Correction: Equation (D3) contained an error and has been fixed.

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References (47)

  1. J. Binney and S. Tremaine, Galactic Dynamics, 2nd ed. (Princeton University Press, Princeton, NJ, 2008).
  2. D. Heggie and P. Hut, The Gravitational Million–Body Problem: A Multidisciplinary Approach to Star Cluster Dynamics (Cambridge University Press, Cambridge, England, 2003).
  3. H. B. Perets and K. M. Kratter, The Triple Evolution Dynamical Instability: Stellar Collisions in the Field and the Formation of Exotic Binaries, Astrophys. J. 760, 99 (2012).
  4. E. Michaely and H. B. Perets, High Rate of Gravitational Waves Mergers from Flyby Perturbations of Wide Black Hole Triples in the Field, Mon. Not. R. Astron. Soc. 498, 4924 (2020).
  5. D. C. Heggie, Binary Evolution in Stellar Dynamics, Mon. Not. R. Astron. Soc. 173, 729 (1975).
  6. M. Valtonen and H. Karttunen, The Three-Body Problem (Cambridge University Press, Cambridge, England, 2006).
  7. V. I. Arnold, V. V. Kozlov, and A. I. Neishtadt, Mathematical Aspects of Classical and Celestial Mechanics, 3rd ed., Encyclopaedia of Mathematical Sciences (Springer-Verlag, Berlin, 2006), Vol. 3, pp. xiv+518, Translated from the Russian original by E. Khukhro.
  8. W. C. Saslaw, M. J. Valtonen, and S. J. Aarseth, The Gravitational Slingshot and the Structure of Extragalactic Radio Sources, Astrophys. J. 190, 253 (1974).
  9. J. G. Hills, Encounters between Binary and Single Stars and Their Effect on the Dynamical Evolution of Stellar Systems, Astron. J. 80, 809 (1975).
  10. J. G. Hills and L. W. Fullerton, Computer Simulations of Close Encounters between Single Stars and Hard Binaries, Astron. J. 85, 1281 (1980).
  11. J. P. Anosova, Dynamical Evolution of Triple Systems, Astrophys. Space Sci. 124, 217 (1986).
  12. Z. P. Anosova and V. V. Orlov, Dynamical Evolution of Equal-Mass Triple Systems in Three Dimensions, Sov. Astron. 30, 380 (1986).
  13. J. G. Hills, Effect of Intruder Mass on Collisions with Hard Binaries. I. Zero-Impact Parameter, Astron. J. 97, 222 (1989).
  14. J. G. Hills, Effects of Intruder Mass on Collisions With Hard Binaries. II. Dependence on Impact Parameter and Computations of the Interaction Cross Section, Astron. J. 103, 1955 (1992).
  15. D. C. Heggie and P. Hut, Binary–Single-Star Scattering. IV. Analytic Approximations and Fitting Formulae for Cross Sections and Reaction Rates, Astrophys. J. Suppl. Ser. 85, 347 (1993).
  16. P. Hut, Binary–Single-Star Scattering. III. Numerical Experiments for Equal-Mass Hard Binaries, Astrophys. J. 403, 256 (1993).
  17. S. Sigurdsson and E. S. Phinney, Binary–Single Star Interactions in Globular Clusters, Astrophys. J. 415, 631 (1993).
  18. S. Mikkola, A Numerical Exploration of the Phase-Space Structure of Chaotic Three-Body Scattering, Mon. Not. R. Astron. Soc. 269, 127 (1994).
  19. J. Samsing, M. MacLeod, and E. Ramirez-Ruiz, The Formation of Eccentric Compact Binary Inspirals and the Role of Gravitational Wave Emission in Binary-Single Stellar Encounters, Astrophys. J. 784, 71 (2014).
  20. N. W. C. Leigh and S. Wegsman, Illustrating Chaos: A Schematic Discretization of the General Three-Body Problem in Newtonian Gravity, Mon. Not. R. Astron. Soc. 476, 336 (2018).
  21. V. Manwadkar, A. A. Trani, and N. W. C. Leigh, Chaos and Lévy Flights in the Three-Body Problem, Mon. Not. R. Astron. Soc. 497, 3694 (2020).
  22. J. J. Monaghan, A Statistical Theory of the Disruption of Three-Body Systems—I. Low Angular Momentum, Mon. Not. R. Astron. Soc. 176, 63 (1976).
  23. J. J. Monaghan, A Statistical Theory of the Disruption of Three-Body Systems—II. High Angular Momentum, Mon. Not. R. Astron. Soc. 177, 583 (1976).
  24. P. E. Nash and J. J. Monaghan, A Statistical Theory of the Disruption of Three-Body Systems—III. Three-Dimensional Motion, Mon. Not. R. Astron. Soc. 184, 119 (1978).
  25. B. Kol, Flux-Based Statistical Prediction of Three-Body Outcomes, Celest. Mech. Dyn. Astron. 133, 17 (2021).
  26. N. C. Stone and N. W. C. Leigh, A Statistical Solution to the Chaotic, Non-hierarchical Three-Body Problem, Nature (London) 576, 406 (2019).
  27. P. Hut and S. Inagaki, Globular Cluster Evolution with Finite-Size Stars—Cross Sections and Reaction Rates, Astrophys. J. 298, 502 (1985).
  28. J. Samsing, M. MacLeod, and E. Ramirez-Ruiz, Formation of Tidal Captures and Gravitational Wave Inspirals in Binary-Single Interactions, Astrophys. J. 846, 36 (2017).
  29. While we were working on this paper, Ref. [25] provided an alternative approximation to the solution of the nonhierarchical three-body problem, which can be continued analytically to the bound case. This solution contains an unknown “emissivity” multiplicative factor, which has not yet been computed and therefore does not constitute a closed-form solution.

  30. Strictly speaking, one needs to normalize this integral so that it has the correct dimensions. This can be done by working in the appropriate system of units—and by multiplying the integral by functions that are symmetric in all three stars—and is therefore unimportant for the analysis presented in this paper.

  31. S. Naoz, The Eccentric Kozai-Lidov Effect and Its Applications, Annu. Rev. Astron. Astrophys. 54, 441 (2016).
  32. The triple is in a cluster, so it is possible that the star escapes even with Es<0, but that does not affect the calculation at present.

  33. The reason it is not exact is that, when converting the integration over Ebin into an integration over abin, one finds that there are now two parameters with dimension of length that can be used to rescale abin for the purposes of dimensional analysis: R and the original semimajor axis a0. Therefore, there is an additional mass dependence hidden here, which Eq. (36) does not account for [but an integration of Eq. (48) over Ebin does].

  34. We remark that one cannot assume that μsv2 is much smaller than Ebin; if we did, then thermal equilibrium would be precluded, as interactions between hard binaries and single stars are known to be a source of heat for globular clusters (see, e.g., Ref. [2]).

  35. Here, we sum up all orders, so this assumption is innocuous insofar as the general model described in this section is concerned. In Sec. 8, we truncate the series at linear order.

  36. B. D. Hughes, Random Walks and Random Environments, Oxford Science Publications (Clarendon Press, Oxford University Press, Oxford, 1995), Vol. 1, pp. xxii+631.
  37. D. C. Heggie, P. Hut, and S. L. W. McMillan, Binary–Single-Star Scattering. VII. Hard Binary Exchange Cross Sections for Arbitrary Mass Ratios: Numerical Results and Semianalytic FITS, Astrophys. J. 467, 359 (1996).
  38. The cross sections were found by integrating the ejection probabilities given angular momentum J (and energy E) over the allowed values of the impact parameter b, using the law of total probability: Each value of b determines the angular momentum J and, thence, the ejection probabilities, which are then integrated to yield the cross section.

  39. W. H. Press and S. A. Teukolsky, On Formation of Close Binaries by Two-Body Tidal Capture, Astrophys. J. 213, 183 (1977).
  40. This is justified by the fact that the amount of angular momentum that goes into the tidal excitations is about r*3/GmΔE [41], which is very small in comparison with the initial orbital angular momentum of the binary, μbinGmbina0.

  41. C. S. Kochanek, The Dynamical Evolution of Tidal Capture Binaries, Astrophys. J. 385, 604 (1992).
  42. A. C. Fabian, J. E. Pringle, and M. J. Rees, Tidal Capture Formation of Binary Systems and X-Ray Sources in Globular Clusters, Mon. Not. R. Astron. Soc. 172, 15 (1975).
  43. P. Heinämäki, H. J. Lehto, M. J. Valtonen, and A. D. Chernin, Chaos in Three-Body Dynamics: Kolmogorov—Sinai Entropy, Mon. Not. R. Astron. Soc. 310, 811 (1999).
  44. We assume that the initial longest distance between stars is abin and that the binary is hard.

  45. A. Lichtenberg and M. Lieberman, Regular and Chaotic Dynamics (Springer-Verlag, New York, 1992).
  46. S. Redner, A Guide to First-Passage Processes (Cambridge University Press, Cambridge, England, 2001), pp. x+312.
  47. The two are not independent, and in the plots, we have kept ηβ constant when varying β; this affects only the low-energy cutoff of the bound case.

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