How do merging supermassive black holes pass the final parsec?
Astrophysicists are puzzling over how pairs of supermassive black holes in merging galaxies close the “final parsec” and actually collide, with ideas ranging from interactions with stars and gas to exotic possibilities like self‑interacting dark matter. Commenters weigh the appeal and limits of invoking dark matter to fix mismatches between theory and observation, debating whether this represents healthy model refinement or epicycle‑like patching in the absence of direct detection. The thread also touches on upcoming gravitational‑wave observatories like LISA, the detectability and risk of rogue black holes, and how units like parsecs arise from observational practice.
Rogue black holes and other intruders
- Some find the idea of ejected supermassive “rogue” black holes terrifying; others argue they’d be harmless and extremely far away.
- Several comments note such an object would be obvious long in advance via gravitational distortions and strong lensing of background stars.
- Small/“micro” black holes are seen as more worrisome because they could be hard to detect and might pass through a system with little warning.
- Clarification: “small” in the article means stellar-mass, not star-sized. A black hole with Earth’s mass would be ~cm-scale and could pass through the solar system with minimal, hard‑to‑attribute effects.
- Some argue an Earth-mass passerby would barely perturb orbits compared with undetected distant dwarf planets; others think there would be measurable disturbances, but brief and localized.
Mechanisms for black hole mergers and the last parsec
- Core issue: dynamical friction brings supermassive black holes to ~1 parsec; gravitational waves efficiently merge them only below ~0.1 parsec. How they bridge that gap on ~100 Myr timescales is debated.
- Standard mechanism: scattering of stars from specific “loss cone” orbits that carry away energy and shrink the binary. Problem: the cone can empty faster than it refills.
- Some work suggests triaxial (non-spherical) galaxies can keep refilling the loss cone; not universally accepted.
- Other proposed contributors: galactic tides shortly after mergers, stars injected from larger radii, and gas disks.
- Gravitational-wave energy loss is agreed to be real but negligible until very small separations; thus the puzzle is “why so fast,” not “how at all.”
- LISA and pulsar timing arrays are highlighted as promising tools to test these ideas.
Dark matter: explanation, epicycles, and alternatives
- One camp welcomes self‑interacting dark matter as a potentially testable way to extract angular momentum from binaries and unify multiple phenomena.
- Another camp sees this as piling on “kludges,” likening dark matter to epicycles: adjustable distributions per galaxy and ever more parameters.
- Disagreement over terminology: some use “dark matter” broadly for any non-luminous mass (e.g., black holes, brown dwarfs), others for new particles (WIMPs, etc.).
- Some insist dark matter remains the most useful framework until a better theory with evidence appears; others argue it’s depressing to tweak an already hypothetical component instead of questioning gravity itself.
- There is debate over whether this specific merger problem really demands new physics, with several stressing that galactic centers are messy and may be mis-modeled rather than fundamentally misunderstood.
Evidence, non-detection, and the search for dark matter
- Direct and indirect detection efforts are noted; each null result shrinks the allowed parameter space.
- One side emphasizes “absence of evidence is not evidence of absence” and sees systematic exploration of parameter space as normal science.
- Others counter with a Bayesian view: every failed search is weak evidence against existing dark matter models, akin to repeatedly failing to find a lost wallet at home.
- Discussion distinguishes “we have no way to detect it” vs. “we are trying but haven’t succeeded,” and notes both statements can simultaneously be true in practice.
Black hole properties, no-hair theorem, and causality
- One answer to “tidal heating” between black holes: classical black holes are externally described only by mass, charge, and spin, so there’s no surface to knead like a planet.
- Another participant objects that the no‑hair theorem strictly applies only to stationary solutions; real astrophysical black holes are dynamic.
- A thought experiment with infalling charge is used to argue that naively treating the black hole as an instantaneously updated point object can imply faster‑than‑light signaling, so care is needed.
- Follow-ups stress that from a distant observer’s frame, infalling matter appears to slow near the horizon, and changes to fields propagate at light speed, preserving causality; the subtleties remain somewhat unresolved in the thread.
Parsecs vs light-years
- Question: why use parsecs rather than light-years, which are more familiar?
- Replies: tradition in astronomy and the link to parallax measurements. A parsec directly encodes distance via the apparent shift of a star by one arcsecond when Earth moves by 1 AU.
- Some note parsecs also serve as a cultural shibboleth rather than offering a compelling practical advantage.
Aether, spacetime, and gravitational waves
- A long subthread compares historical aether theories with modern views of fields and spacetime.
- One position: modern fields and spacetime are effectively “aethers” (pervasive media supporting waves like light and gravitational waves), with LIGO as a scaled‑up successor to the Michelson–Morley interferometer.
- The opposing view: this is mostly semantic; classical aether was a moving, material medium meant to restore Galilean relativity, whereas modern spacetime/fields are Lorentz invariant and don’t constitute “stuff” in the same way.
- Debate touches on whether spacetime can meaningfully be said to “move,” issues of Lorentz invariance, warp bubbles, and how to define a “chunk” of spacetime; participants do not reach consensus.