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| Event horizon | |
|---|---|
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| Name | Event horizon |
| Type | Boundary in spacetime |
| Discovered | 1916 |
| Discoverer | Karl Schwarzschild; later formalized by David Finkelstein |
| Field | General relativity, Astrophysics |
Event horizon The event horizon is the boundary in spacetime surrounding a compact object beyond which events cannot affect distant observers. It appears in solutions of Albert Einstein's Einstein field equations such as the Schwarzschild metric and the Kerr metric, and features centrally in studies by Karl Schwarzschild, Roy Kerr, Subrahmanyan Chandrasekhar, and Roger Penrose. The concept unites work from David Finkelstein, John Wheeler, Stephen Hawking, and Jacob Bekenstein across Princeton University, Cambridge University, and Institute for Advanced Study research traditions.
In general relativity the event horizon is a null hypersurface that separates causally disconnected regions; it is a global concept defined using the causal structure of a spacetime manifold as developed by Roger Penrose, Stephen Hawking, and Wald, Robert M.. For the nonrotating Schwarzschild solution the horizon is located at the Schwarzschild radius associated with mass parameters studied by Karl Schwarzschild and extended by Hermann Weyl. For rotating or charged solutions such as the Kerr metric and Reissner–Nordström metric the horizon structure includes outer and inner null surfaces analyzed in work by Roy Kerr and Hans Reissner. Horizons are characterized by properties like being a Killing horizon in stationary spacetimes explored by B. Carter and by surface gravity defined in theorems by Stephen Hawking and J. M. Bardeen.
Mathematically, an event horizon is the boundary of the causal past of future null infinity, J–(Scri+) in the conformal compactifications used by Penrose, Roger. In asymptotically flat spacetimes the formal definition employs global hyperbolicity and the causal structure developed in texts by Hawking, Stephen and Wald, Robert M.. Calculations use metrics like the Schwarzschild metric, Kerr metric, Reissner–Nordström metric, and coordinates such as Eddington–Finkelstein coordinates introduced by David Finkelstein and Arthur Eddington, as well as Kruskal–Szekeres coordinates credited to Martin Kruskal and George Szekeres. Techniques from differential geometry by Élie Cartan and causal diagrams from Roger Penrose are standard; global existence proofs and singularity theorems involve work by Stephen Hawking and Roger Penrose.
Physically the event horizon marks where escape velocity reaches the speed of light, linking to observational programs at Event Horizon Telescope collaboratives and to imaging results associated with M87* and Sagittarius A* pursued by teams at Harvard-Smithsonian Center for Astrophysics, Max Planck Institute for Radio Astronomy, and MIT Haystack Observatory. Indirect evidence arises from phenomena in X-ray binaries like Cygnus X-1, gravitational wave detections by LIGO and Virgo from mergers cataloged by the LIGO Scientific Collaboration, and accretion physics modeled using approaches from Shakura–Sunyaev and disk simulations at Princeton Plasma Physics Laboratory. Observables include shadow morphology predicted by ray-tracing codes developed by research groups at Max Planck Institute for Astrophysics and numerical relativity teams at Caltech and Cornell University.
Beyond event horizons, relativistic spacetimes admit apparent horizons studied in numerical relativity groups at AEI (Max Planck Institute for Gravitational Physics), trapping horizons analyzed by Sean Hayward, and cosmological horizons such as the particle horizon and cosmic event horizon relevant to Lambda-CDM cosmology developed by collaborations at NASA and European Space Agency. In rotating black holes the presence of an ergosphere and inner (Cauchy) horizon arises in Kerr–Newman solutions explored by Roy Kerr and Ted Newman. Dynamical horizons and isolated horizons were formulated in loop quantum gravity programs at Perimeter Institute and Pennsylvania State University.
Event horizons underpin the laws of black hole thermodynamics first articulated by J. M. Bardeen, B. Carter, and Stephen Hawking, and link to the Bekenstein–Hawking entropy relation proposed by Jacob Bekenstein and Stephen Hawking. Concepts such as surface gravity, Hawking radiation, and quantum field theory on curved spacetime connect to work by S. W. Hawking, N. D. Birrell, and P. C. W. Davies. Debates about unitarity and the information paradox involve proposals like the holographic principle from Gerard 't Hooft and Leonard Susskind, the AdS/CFT correspondence by Juan Maldacena, firewall arguments from Almheiri, Marolf, Polchinski, Sully groups, and evaporation models studied by researchers at Perimeter Institute and Institute for Advanced Study.
Event horizons influence models of active galactic nuclei at Max Planck Institute for Radio Astronomy and National Radio Astronomy Observatory, gravitational wave source modeling by LIGO Scientific Collaboration, and early-universe scenarios examined at CERN and Fermi National Accelerator Laboratory. They affect observational signatures in jet launching theories associated with Blandford–Znajek mechanisms, population synthesis studies by teams at Space Telescope Science Institute, and tests of gravity with pulsar timing arrays like NANOGrav and missions such as Gaia and James Webb Space Telescope.
The idea originated in metrics by Karl Schwarzschild in 1916 and was refined by David Finkelstein in 1958 who clarified causal structure; theoretical foundations were expanded by Roger Penrose and Stephen Hawking with singularity theorems in the 1960s. Further formalism and quantum considerations were developed by Jacob Bekenstein, John Wheeler, Subrahmanyan Chandrasekhar, and later numerical relativity breakthroughs by researchers at Caltech and Cornell University culminating in gravitational wave observations by LIGO that confirmed dynamic horizon behavior.