Event horizon

In astrophysics, an event horizon is a boundary beyond which events cannot affect an observer. Wolfgang Rindler coined the term in the 1950s.[1]

In 1784, John Michell proposed that gravity can be strong enough in the vicinity of massive compact objects that even light cannot escape.[2] At that time, the Newtonian theory of gravitation and the so-called corpuscular theory of light were dominant. In these theories, if the escape velocity of the gravitational influence of a massive object exceeds the speed of light, then light originating inside or from it can escape temporarily but will return. In 1958, David Finkelstein used general relativity to introduce a stricter definition of a local black hole event horizon as a boundary beyond which events of any kind cannot affect an outside observer, leading to information and firewall paradoxes, encouraging the re-examination of the concept of local event horizons and the notion of black holes. Several theories were subsequently developed, some with and some without event horizons. One of the leading developers of theories to describe black holes, Stephen Hawking, suggested that an apparent horizon should be used instead of an event horizon, saying, "Gravitational collapse produces apparent horizons but no event horizons." He eventually concluded that "the absence of event horizons means that there are no black holes – in the sense of regimes from which light can't escape to infinity."[3][4]

Any object approaching the horizon from the observer's side appears to slow down, never quite crossing the horizon.[5] Due to gravitational redshift, its image reddens over time as the object moves closer to the horizon.[6]

In an expanding universe, the speed of expansion reaches — and even exceeds — the speed of light, preventing signals from traveling to some regions. A cosmic event horizon is a real event horizon because it affects all kinds of signals, including gravitational waves, which travel at the speed of light.

More specific horizon types include the related but distinct absolute and apparent horizons found around a black hole. Other distinct types include:

  1. ^ Rindler, Wolfgang (1956-12-01). "Visual Horizons in World Models". Monthly Notices of the Royal Astronomical Society. 116 (6). [Also reprinted in General Relativity and Gravitation, 34, 133–153 (2002), doi: 10.1023/A:1015347106729]: 662–677. doi:10.1093/mnras/116.6.662. ISSN 0035-8711.
  2. ^ Michell, John (1784). "VII. On the means of discovering the distance, magnitude, &c. of the fixed stars, in consequence of the diminution of the velocity of their light, in case such a diminution should be found to take place in any of them, and such other data should be procured from observations, as would be farther necessary for that purpose. By the Rev. John Michell, B.D. F.R.S. In a letter to Henry Cavendish, Esq. F.R.S. and A.S". Philosophical Transactions of the Royal Society of London. 74. The Royal Society: 35–57. Bibcode:1784RSPT...74...35M. doi:10.1098/rstl.1784.0008. ISSN 0261-0523. JSTOR 106576.
  3. ^ Hawking, Stephen W. (2014). "Information Preservation and Weather Forecasting for Black Holes". arXiv:1401.5761v1 [hep-th].
  4. ^ Curiel, Erik (2019). "The many definitions of a black hole". Nature Astronomy. 3: 27–34. arXiv:1808.01507. Bibcode:2019NatAs...3...27C. doi:10.1038/s41550-018-0602-1. S2CID 119080734.
  5. ^ Chaisson, Eric J. (1990). Relatively Speaking: Relativity, Black Holes, and the Fate of the Universe. W. W. Norton & Company. p. 213. ISBN 978-0393306750.
  6. ^ Bennett, Jeffrey; Donahue, Megan; Schneider, Nicholas; Voit, G. Mark (2014). The Cosmic Perspective. Pearson Education. p. 156. ISBN 978-0-134-05906-8.

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