Gibbons–Hawking–York boundary term
E970552
UNEXPLORED
The Gibbons–Hawking–York boundary term is an additional term in the gravitational action of general relativity that ensures a well-defined variational principle in spacetimes with boundaries.
All labels observed (2)
| Label | Occurrences |
|---|---|
| Gibbons–Hawking–York boundary term canonical | 1 |
| Gibbons–Hawking–York boundary term in gravitational action | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T12216705 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
NED1
Entity disambiguation (via context triple)
gpt-5-mini-2025-08-07
Target entity: Gibbons–Hawking–York boundary term Context triple: [Gary W. Gibbons, knownFor, Gibbons–Hawking–York boundary term]
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A.
Gibbons–Hawking temperature
The Gibbons–Hawking temperature is the characteristic thermal radiation temperature associated with the cosmological horizon of de Sitter space, analogous to the Hawking temperature of black holes.
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B.
Einstein–Hilbert action
The Einstein–Hilbert action is the fundamental action in general relativity whose variation yields Einstein’s field equations, expressing gravity as the dynamics of spacetime curvature.
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C.
Bekenstein–Hawking entropy
Bekenstein–Hawking entropy is the thermodynamic entropy associated with a black hole, proportional to the area of its event horizon and fundamental in linking gravity, quantum theory, and thermodynamics.
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D.
Hartle–Hawking no-boundary proposal
The Hartle–Hawking no-boundary proposal is a quantum cosmological model suggesting that the universe is finite but without an initial temporal boundary, replacing the classical Big Bang singularity with a smooth, boundaryless beginning described by quantum gravity.
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E.
Bondi–Metzner–Sachs symmetry
Bondi–Metzner–Sachs symmetry is an infinite-dimensional group of asymptotic spacetime symmetries in general relativity that characterizes the gravitational field at null infinity, especially in the context of gravitational radiation.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
NED2
Entity disambiguation (via description)
gpt-5-mini-2025-08-07
Target entity: Gibbons–Hawking–York boundary term Target entity description: The Gibbons–Hawking–York boundary term is an additional term in the gravitational action of general relativity that ensures a well-defined variational principle in spacetimes with boundaries.
-
A.
Gibbons–Hawking temperature
The Gibbons–Hawking temperature is the characteristic thermal radiation temperature associated with the cosmological horizon of de Sitter space, analogous to the Hawking temperature of black holes.
-
B.
Einstein–Hilbert action
The Einstein–Hilbert action is the fundamental action in general relativity whose variation yields Einstein’s field equations, expressing gravity as the dynamics of spacetime curvature.
-
C.
Bekenstein–Hawking entropy
Bekenstein–Hawking entropy is the thermodynamic entropy associated with a black hole, proportional to the area of its event horizon and fundamental in linking gravity, quantum theory, and thermodynamics.
-
D.
Hartle–Hawking no-boundary proposal
The Hartle–Hawking no-boundary proposal is a quantum cosmological model suggesting that the universe is finite but without an initial temporal boundary, replacing the classical Big Bang singularity with a smooth, boundaryless beginning described by quantum gravity.
-
E.
Bondi–Metzner–Sachs symmetry
Bondi–Metzner–Sachs symmetry is an infinite-dimensional group of asymptotic spacetime symmetries in general relativity that characterizes the gravitational field at null infinity, especially in the context of gravitational radiation.
- F. None of above. chosen
Referenced by (2)
Full triples — surface form annotated when it differs from this entity's canonical label.
this entity surface form:
Gibbons–Hawking–York boundary term in gravitational action