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Black Hole Formation and Growth: Simulations in General Relativity

arXiv preprint arXiv:0711.1537, S. L. Shapiro (2007)

A clear bell rings in the paper: large computer simulations in full general relativity can now trace how black holes form, how they grow, and how they can power bright bursts.


Key Concepts – the Lanterns the Authors Carry

  • Black Hole (an object so dense light cannot escape)
  • Hypermassive Neutron Star (HMNS) (a heavy, fast-spinning dead star)
  • Magnetohydrodynamics (MHD) (how magnetic fields move hot gas)
  • Equation of State (EOS) (how dense matter behaves)

Guiding Questions

  1. How do different stellar deaths and mergers make black holes?
  2. How do those holes then gain mass?
  3. Can these processes explain short and long gamma-ray bursts and the existence of early supermassive black holes?

The study gathers and summarizes many recent simulations to show the routes.


Tools – Maps of Spacetime Solved on a Computer

  • The 3+1 split and BSSN scheme recast Einstein’s equations so the computer can follow them stably (p. 2–3).
  • Simulations include
    • Neutron star pairs meeting,
    • Strongly magnetized, differentially rotating HMNSs,
    • Collapsing massive stars,
    • Tiny early black hole seeds growing by gas falling in (p. 4–11).

Results – Patterns That Emerge

1. Neutron-Star Mergers

Total Mass ConditionOutcome
Above ~2.5–2.7 M☉Prompt collapse to a black hole
Below ~2.5–2.7 M☉HMNS survives for ~100 ms → delayed collapse → short burst of gravitational waves

2. Magnetized HMNS “Clockworks”

  • Process: Magnetic winding & instabilities move angular momentum outward
  • Timescale: Collapse after ≈66 rotation periods
  • Final State:
    • Black hole ≈0.9 M☉
    • Hot, accreting torus ≈0.1 M☉
    • Field lines focused along spin axis
  • Energy Output: Torus lives ~10 ms, emits ~10⁵⁰ ergs in neutrinos before being swallowed

“All these properties make this system a promising central engine for a short-hard GRB.”


3. Collapsing Very Massive Stars

  • Outcome:
    • Black hole mass: M_h ≈ 0.95 M☉, spin: J_h/M_h² ≈ 0.7
    • Thick, hot torus feeds turbulent, episodic accretion
    • Magnetic fields collimate along axis

Described as a “viable candidate for the central engine of a long-soft GRB.”


4. Growing Small Seeds into Supermassive Beacons

  • Key: Efficiency ε_M of turning mass into light matters
  • Turbulent MHD disk: ε_M ≈ 0.19 → growth feasible
  • Standard thin disk: ε_M ≈ 0.32 or higher → growth harder or impossible

Caveats – Careful and Quiet About Limits

Results depend on

  • The assumed EOS,
  • The initial magnetic strength,
  • Simplifications such as axisymmetry and frozen spacetime.

The authors call for more detailed relativistic MHD work—including radiation effects—to sharpen the map.


Metaphorical Closing

Think of these simulations as a set of lanterns along a dark path.
Each lamp—merger, magnetized collapse, accreting disk—shows a different route to a black hole and a different way to light the sky.

Together, they stitch local, relativistic physics into the larger story of how black holes grow and power bursts across the universe.