Kerr Ringdown Frequency Calculator

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What this calculator computes

After a black hole merger (or any strong perturbation), the remnant relaxes to a stationary Kerr black hole by emitting gravitational radiation in a superposition of quasinormal modes (QNMs). Each mode behaves like a damped oscillator with a complex angular frequency ω. The real part sets the oscillation frequency and the imaginary part sets how quickly the signal decays.

This tool estimates the dominant (“fundamental”) Kerr ringdown mode—commonly written =m=2,n=0—and reports:

Inputs

Equations used (semi-analytic fit)

The calculator uses a widely-cited approximate fit (originating with Echeverria and later refinements) for the fundamental =m=2,n=0 mode. In terms of mass M and dimensionless spin a, the frequency is approximated by

f = c3 2πGM [ 1 0.63 (1a) 0.3 ]

The quality factor is approximated by

Q=2(1a)0.45.

Given f and Q, the damping time is computed as

τ=Qπf.

Interpreting the results

Worked example (using the default inputs)

Suppose the remnant has mass M=30M and spin a=0.7.

  1. Compute the spin-dependent bracket term:
    (1a)0.3=(0.3)0.30.697, so 10.63(1a)0.310.63×0.6970.561.
  2. The mass scaling factor c32πGM for 30 M is about 1.08 kHz.
  3. Frequency: f1.08kHz×0.561610Hz.
  4. Quality factor: Q=2(1a)0.45=2(0.3)0.453.44.
  5. Damping time: τ=Qπf3.44π×610 s1.8 ms.

Interpretation: a kHz ringdown is squarely in the ground-based band; the millisecond decay time indicates only a handful of visible cycles unless the signal is very loud.

How mass and spin change ringdown (quick comparison)

Parameter change Effect on frequency f Effect on quality factor Q Effect on damping time τ
Increase mass M (fixed spin) Decreases (~1M) ≈ no change (in this fit) Increases (~M)
Increase spin a (fixed mass) Increases (moderately) Increases Usually increases (because Q grows faster than f)
Spin near 0 (slow rotation) Lower “pitch” Lower Q Shorter-lived ringdown
Spin near 1 (near-extremal) Higher “pitch” Higher Q Longer-lived ringdown

Assumptions & limitations (read before using)

FAQ

Which ringdown mode is used?

The dominant fundamental Kerr mode =m=2,n=0, often the strongest component in binary black hole mergers.

Why does spin change the ringdown frequency and decay?

Spin changes the Kerr spacetime’s characteristic scales (e.g., the effective potential governing perturbations). Higher spin shifts the mode spectrum to higher real frequency and typically reduces damping (higher Q).

Is this the same as the “chirp” frequency?

No. The chirp frequency describes the inspiral and merger evolution. Ringdown is the late-time, approximately exponentially damped oscillation of the remnant black hole.

How accurate are these numbers?

They are intended as first-order estimates. For precision work, use up-to-date QNM fitting formulae (or direct numerical relativity / perturbation solvers) and include multiple modes and redshift.

How do I compare this to detector bands?

Ground-based detectors are most sensitive from tens to a few thousand Hz; space-based detectors target much lower frequencies (milliHertz). Always compare against a specific detector noise curve and include redshift for distant sources.

Enter parameters and compute.

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