Event
Horizons 

In General > s.a. black holes / boundaries and holography
in field theory; quantum
spacetime; Rigidity; Trapped Surface.
$ Of a worldline: The
past (future) event horizon is the boundary of the future (past) of the worldline.
$ Of a spacetime: The
boundary of the past of \(\cal I\)^{+},
\(\cal H\) = ∂(I^{ –}(\(\cal I\)^{+}))
(the future event horizon is the boundary of the future of \(\cal I\)^{–});
It is a global concept, defining from which points one can reach (null) infinity.
* Relationships: Its
existence is equivalent to \(\cal I\)^{–} (\(\cal I\)^{+})
being spacelike (> see de sitter spacetime).
* Properties: They are
always null hypersurfaces; Their area always increases; They either coincide
or are outside the apparent horizon (not true?).
* Remark: Being global
properties, they are in general difficult to calculate, except when they can
be shown to coincide with a Killing horizon or some other
locally defined surface. [Defined by retarded time u = ∞.]
@ References: Baccetti et al a1706GRF [existence?].
Geometry and Topology > s.a. black
holes; blackhole
types [toroidal]; topology change [censorship]
@ Geometry: Chruściel et al AHP(01)gq/00 [area], JGP(02)gq/00 [differentiability],
CQG(06)gq/05 [no
degenerate components].
@ Topology: Huang & Liang PLA(95) [torus]; Siino PRD(98)gq/97, PRD(99)gq/97.
@ Related topics: Booth & Martin PRD(10)a1007 [geometrical
measure of the distance between apparent and event horizons, and Vaidya spacetime]; Chung PRD(11)a1011 [dynamics of diffeomorphism degrees of freedom]; Brill G&C(14) [dynamic changes in a black hole horizon as it forms and settles]; Shi & Mei a1611 [extended BMSlike symmetries].
Related Topics > s.a. Firewall; Fuzzball; gravitational thermodynamics.
* Thermodynamics: Thermal properties of a static horizon (like its entropy or heat content) can be obtained either from the surface term of the EinsteinHilbert action or by evaluating the Noether charge, corresponding to the diffeomorphisms generated by the timelike Killing vector field.
* Alternatives: To resolve some puzzles arising from properties of quantum field theory in the presence of horizons, some physicists have proposed that the equivalence principle (or "no drama" scenario) does not hold near the surface of a black hole and the event horizon is replaced by a "firewall" (Almheiri, Marolf, Polchinski, and Sully) which would cause any observer who reaches the firewall to burn and not be able to cross to the other side, or a "fuzzball", motivated by string theory.
@ Thermodynamics: Gibbons & Hawking PRD(77);
Fulling & Ruijsenaars
PRP(87);
Davies CQG(87),
CQG(88), AIHP(88),
comment Raychaudhuri CQG(90);
Jensen PRD(95)
[stability]; Massar & Parentani NPB(00)gq/99;
Padmanabhan IJMPD(04)gq [and
gravity as elasticity]; Zhou et al PLB(07)
[second law in accelerating universe]; Majhi & Padmanabhan EPJC(13)a1302 [from infinitesimal coordinate transformations]; Widom et al a1602 [and gravitational vacuum tension]; > s.a. horizons.
@ And particle motion: Oliveira a1107 [velocity of test particles at the event horizon, pedagogical].
@ Horizon wave functions: Casadio a1310proc [and effective gup]; Casadio et al a1509 [in various dimensions].
@ Quantum effects: Hájíček PLB(86);
Padmanabhan PLB(86);
Sorkin in(96)gq/97 [wrinkling
below threshold scale]; Chapline et al IJMPA(03)gq/00 [phase
transition]; 't Hooft gq/04ln
[and quantum information]; Bojowald et al CQG(11) [definitions in modified spacetime structures]; Susskind a1402 [and computational complexity]; AlonsoSerrano et al PRD(14)a1410 [unitarity is not preserved in individual regions separated by horizons]; > s.a. correlations; quantum
black holes.
@ Other properties: Bergamin et al CQG(06)ht/05 [physicaltogaugedegreeoffreedom
conversion]; Mathur IJMPD(13) [what happens at the horizon].
@ In modified gravity theories: Berglund et al PRD(12) ["universal horizon" mechanics].
@ Numerical methods: Libson et al PRD(96); > s.a. models
in numerical general relativity.
@ Cosmological: Kaloper et al PLB(04) [observational implications].
@ Observational evidence: Barbieri & Chapline PLB(12) [experimental signature for the absence of an event horizon]; Bambi SWJ(13)a1205 [nonobservation of radiation vs ergoregion instability]; Visser PRD(14)a1407 [(non)observability]; Cardoso & Pani a1707; > s.a. blackhole phenomenology.
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send feedback and suggestions to bombelli at olemiss.edu – modified 11
jul
2017