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Antidesitter space

Antidesitter space is a maximally symmetric , simply connected , pseudo-Riemannian manifold of constant negative curvature . It can be considered a pseudo-Riemannian analogue.n {\ displaystyle n} n -dimensional hyperbolic space . Named as opposed to de Sitter space , usually denotedAdSn {\ displaystyle AdS_ {n}} AdS_ {n}

In the language of the general theory of relativity , the antidesitter space is the most symmetric solution of the Einstein equations in vacuum with a negative cosmological constantΛ {\ displaystyle \ Lambda} \ Lambda . The metric of such a space:

ds2=oney2(dt2-dy2-∑idxi2){\ displaystyle ds ^ {2} = {\ frac {1} {y ^ {2}}} \ left (dt ^ {2} -dy ^ {2} - \ sum _ {i} dx_ {i} ^ { 2} \ right)} {\ displaystyle ds ^ {2} = {\ frac {1} {y ^ {2}}} \ left (dt ^ {2} -dy ^ {2} - \ sum _ {i} dx_ {i} ^ { 2} \ right)} .

Antidesitter space is represented as a one-sheeted hyperboloid embedded in a multidimensional Minkowski space [1] .

Notes

  1. ↑ Angsachon Tosaporn. Elements of the special and general theory of relativity in R- space. - SPb .: SPBU, 2013

Links

  • Space-time of negative curvature. // Juan Maldacena. The illusion of gravity. - Elements (Reprint from the journal "In the World of Science" No. 2, 2006)
  • Lecture 8. The Friedman Universe. The space of (anti-) de Sitter // M.O. Katanaev, Doctor of Physics and Mathematics n . Special course “General Theory of Relativity and Geometric Theory of Defects” - M. Steklov Mathematical Institute, 2015
Source - https://ru.wikipedia.org/w/index.php?title=Anti-desitter space &oldid = 93816891


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