Two neutron stars collide, and the space around them ripples like the surface of a pond after a stone is thrown. Huge gravitational wave detectors catch these ripples. If the collision also launches a narrow beam of gamma rays, space telescopes see it as a short gamma-ray burst.
Both signals tell the same story, but they don't always match in numbers. Recent data from LIGO, Virgo, and KAGRA show fewer neutron star mergers than expected from the number of gamma-ray bursts. Astrophysicists tested whether this discrepancy can be explained if the plasma jets from mergers are not emitted in all directions but only at certain angles.
It turns out that if more than half of neutron star mergers produce jets with an opening angle of at least 10 degrees, the numbers of gamma-ray bursts and gravitational wave signals match. But for narrow jets of 6 degrees, the gamma-ray burst rate would need to be lower than some estimates suggest.
Neutron star–black hole mergers also contribute, but only a small fraction — about 6–16% of all short gamma-ray bursts. They can't explain the highest burst rate estimates, but they don't disrupt the overall picture.
So far, the data don't contradict each other. Mergers of two neutron stars remain the primary sources of short gamma-ray bursts, and their jets tend to be wide rather than narrow.
as written by the authors arXiv:2604.05046
Gravitational wave (GW) and short Gamma Ray Burst (sGRB) observations provide us with complementary views of compact object mergers. The paucity of binary neutron star merger (BNS) detections in the latest LIGO/Virgo/KAGRA (LVK) observing run raises the question of whether the GW merger rates are sufficient to explain the observed sGRB rate with compact object mergers alone. We investigate this connection using the latest merger rate constraints from the fourth LVK observing run (O4) and published estimates of the local sGRB rate density. For an observed sGRB rate density of $$ \sim 1-7~\mathrm{Gpc^{-3}\,yr^{-1}}$$, if $$>55\%$$ of BNS mergers can successfully launch a jet, we find that the current LVK BNS merger rate can be reconciled with a sGRB merger population containing a significant fraction of relatively wide jets with core half-opening angles $$\theta_j \geq 10^\circ$$. Meanwhile, a narrow jet population ($$\theta_j \sim 6^\circ$$) can only be matched with the O4 neutron star merger rate estimates for an observed sGRB rate density of $$\lesssim 1~\mathrm{Gpc^{-3}\,yr^{-1}}$$, which is broadly consistent with several of the latest available estimates. We also find that neutron star-black hole mergers (NSBH) are expected to be a subdominant component of the sGRB population compared to BNS mergers, and they cannot help reconcile some of the highest available sGRB rate ($$ >7~\mathrm{Gpc^{-3}\,yr^{-1}}$$) with the GW rate estimates. However, they can still substantially contribute to the sGRB population, comprising $$\sim 6-16\%$$ of it for an observed sGRB rate density of $$\sim 1-3~\mathrm{Gpc^{-3}\,yr^{-1}}$$. Overall, our results indicate that present GW and sGRB observations remain broadly consistent with BNS mergers as the main progenitors of sGRBs.
A short gamma-ray burst lasts less than two seconds, yet in that time it releases as much energy as the Sun will emit over its entire lifetime.
In the movie Interstellar, the merger of black holes produces gravitational waves that the characters use for communication — a principle similar to what we use to observe neutron star mergers.