Article ID Journal Published Year Pages File Type
1840645 Nuclear Physics B 2014 46 Pages PDF
Abstract

A lot of confusion surrounds the issue of black hole complementarity, because the question has been considered without discussing the mechanism which guarantees unitarity. Considering such a mechanism leads to the following: (1) The Hawking quanta with energy E of order the black hole temperature T   carry information, and so only appropriate processes involving E≫TE≫T quanta can have any possible complementary description with an information-free horizon; (2) The stretched horizon describes all possible black hole states with a given mass M  , and it must expand out to a distance sbubblesbubble before it can accept additional infalling bits; (3) The Hawking radiation has a specific low temperature T  , and infalling quanta interact significantly with it only within a distance sαsα of the horizon. One finds sα≪sbubblesα≪sbubble for E≫TE≫T, and this removes the argument against complementarity recently made by Almheiri et al. In particular, the condition E≫TE≫T leads to the notion of ‘fuzzball complementarity’, where the modes around the horizon are indeed correctly entangled in the complementary picture to give the vacuum.

Related Topics
Physical Sciences and Engineering Mathematics Mathematical Physics
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