How Black Holes Lose Their Spin in an Extended Theory of Gravity ✎ express

Original: "Angular momentum flux through post-Newtonian order for noncircular nonspinning black-hole binaries in Einstein-Maxwell-dilaton theory"
· Qi Tan, Peng-Cheng Li
arXiv:2607.17887 · 2026-07-20 · arXiv non-exclusive · independent analysis · 2 min
Physicists have calculated how invisible fields carry away angular momentum from a pair of black holes on non-circular orbits.

A pair of black holes circles in a dance, gradually drawing closer. They lose energy and spin — a process known as angular momentum radiation. In standard Einstein theory, only gravitational waves carry away angular momentum. But what if nature has additional fields?

The authors of the study took a more complex theory — Einstein–Maxwell–dilaton. In addition to the familiar gravitational field, there are also a scalar field (the dilaton) and an electromagnetic field. They calculated how these three channels together carry away angular momentum from a pair of non-spinning black holes moving not in circles but along elongated orbits. The calculation was done to first post-Newtonian order, like a correction to Newtonian physics for fast and massive objects.

The scalar and electromagnetic fields start carrying away angular momentum already at the dipole — the simplest type of radiation. Gravitational radiation, by contrast, only kicks in at the quadrupole, which is weaker at low speeds.

The result doesn't hang in the air. It exactly reproduces known limits: when the orbit is nearly circular, the balance relation holds; if you remove the dilaton, you get pure general relativity; and if the fields are very weak, their contribution naturally fades away. Together with the previously calculated energy flux, these data give a complete picture of the losses — a foundation for future models of eccentric orbit evolution and precise calculation of the phases of gravitational waves.

The more elongated the orbit, the more noticeable the contribution of scalar and electromagnetic radiation. On a circular orbit, they barely show up.

So the dance of black holes losing spin through invisible channels becomes a little clearer. And when detectors catch a signal from a real pair, we'll be able to check — does a scalar field exist in nature, or is gravity alone?

The scalar field (dilaton) in this theory is like an invisible "third dancer" that speeds up the loss of spin of black holes, while itself remaining unnoticed.

Scientists
Albert EinsteinBarry BarishKip ThorneRichard FeynmanRussell HulseHenri Poincaré
Concepts
reissner nordstrom black hole schwarzschild black hole gravitational instanton schwarzschild metric Einstein field equations anomalous hall effect Maxwell's equations kerr metric tidal charge ferron hall effect energy momentum tensor einstein instanton inflaton quadrupole moment no-hair theorem quadrupole radiation formula classical gravity angular momentum spin orbit coupling