black hole no-hair theorem
E6813
The black hole no-hair theorem is a principle in general relativity stating that stationary black holes are completely characterized by only a few macroscopic parameters—mass, electric charge, and angular momentum—regardless of the details of the matter that formed them.
All labels observed (3)
| Label | Occurrences |
|---|---|
| no-hair theorem | 3 |
| black hole no-hair theorem canonical | 1 |
| no-hair theorem for black holes | 1 |
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
no-hair theorem
ⓘ
theorem in general relativity ⓘ |
| appliesTo | stationary black holes ⓘ |
| assumes |
Einstein field equations
ⓘ
absence of matter fields outside the black hole other than electromagnetic field ⓘ asymptotic flatness of spacetime ⓘ classical, non-quantum description of gravity ⓘ cosmic censorship hypothesis in many formulations ⓘ stationarity ⓘ |
| category |
black hole physics
ⓘ
mathematical relativity ⓘ |
| concerns | classical black holes ⓘ |
| consequence | all stationary, asymptotically flat, electrovac black holes are described by the Kerr–Newman family of solutions ⓘ |
| contrastsWith | dependence on microscopic details of collapsing matter ⓘ |
| excludes | additional classical hair such as higher independent multipole moments ⓘ |
| field | general relativity ⓘ |
| hasExtension | no-hair conjectures for additional fields ⓘ |
| hasImplication | information about infalling matter is not encoded in additional classical observables outside the horizon ⓘ |
| hasLimitation |
does not fully address dynamical or non-stationary black holes
ⓘ
may not apply in non-asymptotically flat spacetimes such as with cosmological constant ⓘ |
| hasNameOrigin | metaphor that black holes have no hair, meaning no additional distinguishing features ⓘ |
| hasStatus | rigorously proven only under specific assumptions ⓘ |
| holdsFor |
charged rotating black holes described by the Kerr–Newman metric
ⓘ
non-rotating uncharged black holes described by the Schwarzschild metric ⓘ uncharged rotating black holes described by the Kerr metric ⓘ |
| implies |
black holes have no additional independent multipole moments beyond those determined by mass, charge, and angular momentum
ⓘ
details of the matter that formed a black hole are not observable from outside except through mass, charge, and angular momentum ⓘ |
| influences |
black hole information paradox
ⓘ
black hole thermodynamics ⓘ |
| involves |
angular momentum dipole moment
ⓘ
electric monopole moment ⓘ mass monopole moment ⓘ |
| isAbout | macroscopic characterization of black holes ⓘ |
| mayBeModifiedBy | quantum effects ⓘ |
| mayFailIn | theories with additional long-range fields ⓘ |
| motivates | search for observational signatures of deviations from Kerr geometry ⓘ |
| parameter |
angular momentum
ⓘ
electric charge ⓘ mass ⓘ |
| relatedConcept |
Israel–Carter–Robinson uniqueness theorems
ⓘ
Kerr–Newman black hole ⓘ |
| relatesTo |
black hole uniqueness theorems
ⓘ
event horizon ⓘ |
| statesThat | a stationary black hole is completely characterized by a small set of macroscopic parameters ⓘ |
| testedBy | ringdown phase observations of binary black hole mergers ⓘ |
| usedIn |
astrophysical modeling of black holes
ⓘ
tests of general relativity with gravitational waves ⓘ |
Referenced by (5)
Full triples — surface form annotated when it differs from this entity's canonical label.
this entity surface form:
no-hair theorem
this entity surface form:
no-hair theorem
this entity surface form:
no-hair theorem
this entity surface form:
no-hair theorem for black holes