Gravitational Waves with a Space-Time Correction ✎ express

Original: "Gravitational wave propagation in Ho\v{r}ava-Lifshitz gravity"
arXiv:2607.17431 · 2026-07-19 · arXiv non-exclusive · independent analysis · 2 min
A tiny addition to the laws of gravity changes the height and rhythm of ripples from distant black holes.

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When two black holes merge far away, we receive a tremor of space — gravitational waves. Usually, they are described by Einstein's equations, but what if gravity works differently at the tiniest distances? The authors took one such hypothesis — Hořava–Lifshitz gravity. In it, a term with the fourth power of the wave number (k⁴) is added to the familiar wave equation. It's as if a stretched string, besides its usual elasticity, gained an extra stiffness noticeable only at very rapid oscillations.

It turns out that such an addition does not break the shape of the waves: the two standard polarizations (“plus” and “cross”) are preserved, do not mix, and do not split by helicity. But the signal's amplitude and phase begin to depend on frequency. The higher the frequency, the stronger the correction. For a pair of black holes on a circular orbit, this means that the gravitational wave signal reaches us slightly quieter and with a small time shift, like an echo that not only fades but also slightly changes its pitch.

The correction to the amplitude is proportional to the square of the frequency: Δh/h ≈ –8π²α f². For typical LIGO signals (f ~ 100 Hz) and α ~ 10² eV⁻², the effect is fractions of a percent.

The scientists derived formulas for the energy flux and total luminosity of such a system, as well as for the gradual increase in signal frequency — the so-called chirp. Comparing with the GWTC-4.0 catalog, they obtained a constraint on the parameter α: from –620 to +190 in units of inverse square electronvolt. This means that if the extra stiffness of space exists, it is very small, but already not zero within measurement accuracy.

The accumulated phase correction in terms of frequency dependence corresponds to a contribution of the order of the third post-Newtonian approximation (3PN). This is a very subtle effect, but it is fundamentally distinguishable from ordinary relativistic corrections.

LIGO detectors sense mirror displacements of thousandths of a proton diameter — roughly like the distance to the nearest star changing by the thickness of a human hair.

In Carl Sagan's novel "Contact," the heroine hears a rhythmic signal from space that turns out to be a message from an alien civilization encoded in the modulation of gravitational waves.

\omega^{2}=k^{2}+\alpha k^{4}
modified dispersion relation for gravitational waves: ω is frequency, k is wave number, α is a small parameter of the theory
Scientists
Albert EinsteinBarry BarishKip ThorneRichard FeynmanRussell HulseStephen Hawking
Concepts
gravitational wave propagation gravitational waves quadrupole radiation formula wave amplification gw190814 Klein-Gordon equation fr gravity teleparallel gravity gravitational wave frequency gravitational wave echo black hole ringdown kagra black hole superradiance wave propagation fq gravity direct waves gw170817 gwtc