Gibbons–Hawking space
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In mathematical physics, a Gibbons–Hawking space, named after Gary Gibbons and Stephen Hawking, is essentially a hyperkähler manifold with an extra U(1) symmetry.[1] (In general, Gibbons–Hawking metrics are a subclass of hyperkähler metrics.[2]) Gibbons–Hawking spaces, especially ambipolar ones,[3] find an application in the study of black hole microstate geometries.[1][4]
See also
References
- ↑ 1.0 1.1 Mathur, Samir D. (22 January 2009). "The fuzzball paradigm for black holes: FAQ". Ohio State University. p. 20. http://www.physics.ohio-state.edu/~mathur/faq2.pdf. Retrieved 16 April 2012.
- ↑ Wang, Chih-Wei (2007). Five Dimensional Microstate Geometries. p. 67. ISBN 978-0-549-39022-0. https://books.google.com/books?id=Q-8vohfZZPMC&pg=PA67. Retrieved 16 April 2012.
- ↑ Bellucci, Stefano (2008). Supersymmetric Mechanics: Attractors and Black Holes in Supersymmetric Gravity. Springer. p. 5. ISBN 978-3-540-79522-3. https://books.google.com/books?id=eQMz40csKqsC&pg=PA5. Retrieved 16 April 2012.
- ↑ Bena, Iosif; Nikolay Bobev; Stefano Giusto; Clement Ruefa; Nicholas P. Warner (March 2011). "An infinite-dimensional family of black-hole microstate geometries". Journal of High Energy Physics (International School for Advanced Studies.!) 3 (22): 22. doi:10.1007/JHEP03(2011)022. Bibcode: 2011JHEP...03..022B.
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