property

scalar hair black hole

Additional observable parameters beyond mass, charge, and angular momentum in certain black hole solutions.
12 related articles · 2 formulas

Description

In classical general relativity, black holes are famously 'bald': their external appearance is completely determined by just three parameters — mass, electric charge, and angular momentum. This is the no-hair theorem. However, when additional fields (like scalar fields) are present, certain black hole solutions acquire extra 'hair' — observable parameters beyond the standard trio. These hairy black holes challenge the simplicity of the bald picture and open a rich landscape of exotic solutions.

History

The no-hair theorem was conjectured in the 1960s by Werner Israel and others, with rigorous proofs for electrovacuum solutions. Hairy black holes were discovered in the 1990s in theories with non-minimally coupled scalar fields, notably by Bekenstein and others.

How it works

The no-hair theorem holds under specific assumptions, such as the absence of matter fields or certain energy conditions. When a scalar field is coupled to gravity in a non-minimal way, or when the field has a mass or self-interaction, stable configurations can exist where the scalar field is non-trivial outside the horizon. This scalar 'hair' modifies the spacetime geometry and can affect phenomena like gravitational wave emission, black hole shadows, and orbital dynamics of nearby stars.

In practice

Hairy black holes are studied in the context of modified gravity theories and as potential observational targets for gravitational wave detectors and black hole imaging, where deviations from the bald solution could reveal new physics.

Fun fact

Some hairy black hole solutions are unstable and can 'burst' like soap bubbles, transitioning to a bald state or another configuration.

Concept graph →

Formulas

$$M_{\text{PBH}} \propto k_p^{-2}$$
Primordial black hole mass scales with perturbation scale.
What is in the formula
M_PBHvariablePrimordial black hole mass — mass kilogram
k_pvariablePerturbation wavenumber — wavenumber per metre
∝operatorProportional to — proportionality
m_{\rmpbh}\approx30m_\odot(\frac{g_*}{10.75})^{-1/6}(\frac{k_p}{2.9*10^5{\rmmpc}^{-1}})^{-2} · 2607.01818
$$a = \frac{Jc}{GM^2}$$
Spin parameter of a black hole, normalized by mass.
What is in the formula
avariableDimensionless spin parameter — dimensionless spin parameter
JvariableAngular momentum of the black hole — angular momentum kilogram metre squared per second
MvariableMass of the black hole — mass kilogram
cconstantSpeed of light in vacuum, a fundamental constant of nature. — speed of light = 299792458 metre per second
GconstantNewtonian constant of gravitation, determining the strength of gravity. — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
a=\frac{jc}{gm^2} · 2607.06902
a_*=\frac{jc}{gm^2} · 2607.14218

Related articles · 12

General Relativity2026-08-072 minarXiv:2608.07237express
How Gravitational Waves Expose Black Hole Impostors
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HEP Theory2026-08-062 minarXiv:2608.06016express
Hairy Black Holes and Strings
A black hole is not just a dark sphere. In string theory, it can grow 'hair'—extra scalar fields such as the axion and the dilaton. These fields gently alter the geometry of space around the hole.
General Relativity2026-08-011 minarXiv:2608.00557express
Cauchy Horizon: Why It Survived
A black hole is like a perfectly smooth sphere. It has no features — only mass, charge, and spin. This rule is called "no-hair." But nature loves to complicate things: sometimes a cloud of a scalar field (a special field described by a single number at each point) spontaneously appears around a black hole.
General Relativity2026-07-261 minarXiv:2607.23644express
A Black Hole with Two Thermometers
A pot of boiling water is covered with two lids — an inner and an outer one. The thermometer under each shows its own temperature, but their harmonic mean (a special averaging method where you add the reciprocals) always remains unchanged. Heat seems to obey an invisible rule.
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Quantum Whisper Wakes a Black Hole
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General Relativity2026-06-291 minarXiv:2606.30865express
Black Holes Grow a Fur Coat on the Fly
Two black holes race past each other like Formula 1 cars on opposite lanes. In standard general relativity, they remain 'bald'—no extra fields appear around them. But if you add a scalar field to the equations (something like an invisible fog permeating space), the rules change.
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Black Hole with a Monopole: A Thermal Shield
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General Relativity2026-06-192 minarXiv:2606.21549express
Charge Turns Bald Black Holes Hairy
Two magnets collide in a dark room, stick together into a clump, and a dull thud echoes. Black holes behave much the same way, except instead of magnets they carry electric charge, and instead of a thud, there's a burst of gravitational waves. But there's a third player in this story — an invisible field that physicists call scalar.
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When a Weak Voice Outshouts a Loud One
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General Relativity2026-04-242 minarXiv:2604.22437express
Hairy Black Holes Pop Like Soap Bubbles
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General Relativity2026-04-171 minarXiv:2604.15758express
Black Hole Without a Singularity
An ordinary black hole resembles a funnel, at whose center spacetime plunges into a point — a singularity. There, density becomes infinite and the laws of physics break down. But what if, instead of a plunge, there were a smooth bottom inside? The authors of the study constructed exactly such a model.
General Relativity2026-03-212 minarXiv:2603.20596express
What Black Holes Without Singularities Hide: From Hypotheses to Testing
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