Using Schur-Weyl duality relations between unitary groups and symmetric groups, these questions translate into structural questions about the centres of symmetric group algebras. The information theoretic study of LLM geometries and superstars in the dual AdS5× S5 background has raised a number of questions about the distinguishability of Young diagrams when a finite set of Casimirs are known. ![]() This leads to two related puzzles: (1) How does the effective factorization of interior and exterior degrees of freedom emerge in gravity?, and (2) How does the underlying degeneracy of states wind up having a geometric realization in the horizon area and in properties of the singularity? We explore these puzzles in the context of an incipient black hole in the AdS/CFT correspondence, the microstates of which are dual to half-BPS states of the $$ \mathcal \) = 4 SYM with U(N) gauge symmetry, the multiplicity of half-BPS states with fixed dimension can be labelled by Young diagrams and can be distinguished using conserved charges corresponding to Casimirs of U(N). doi:10.Black holes have an enormous underlying space of microstates, but universal macroscopic physics characterized by mass, charge and angular momentum as well as a causally disconnected interior. Kouveliotou, et al., Astrophysical Journal Letters, Vol. Fraley, Astrophysics and Space Science, Vol. Katz, “The Biggest Bangs,” Oxford University Press, Oxford, 2002, p. Piran, Monthly Notices of the Royal Astronomical Society, Vol. Krasnoholovets, The International Journal of Systems and Cybernetics, Vol. Krasnoholovets, Journal of Modern Physics, Vol. Krasnoholovets, Progress in Physics, Vol. Mottola, Proceedings of the National Academy of Sciences of the United States of America, Vol. Unlikeīlack holes and gravastars that lose information, singularity-free superstars that Region and the phase boundary from the super matter core, resulting in GRB toĪccount for the observed high amount of gamma rays and the observed complex light curves in GRBs. Eventually, the stellar breakup occurs to detach the ordinary matter ![]() Ordinary matter region into the super matter, and decreases the ordinary matter Super matter core by converting the in falling ordinary energy and matter from the Matter core and the ordinary matter region. A pre-superstar contains the super matterĬore, the ordinary matter region, and the thin phase boundary between the super Reaches the critical extreme density during the stellar collapse, the stellarĬore is transformed into the super matter core with extreme force fields and ordinaryįorce fields without singularity. Manifested as the bonds among electrons in a superconductor and among atoms in aīose-Einstein condensate. Interacting energy) at infinite density in ordinary force fields. Inactivation of force fields at absolute zero and singularity (infinite (electromagnetic, weak, strong, and gravitational forces) to prevent the Only at an extremely low temperature above absolute zero or anĮxtremely high density below infinite density, extreme force fields are shortrange,Īnd located in between a particle and its ordinary force fields Infinite density, respectively, based on the uncertainty principle. Non-zero momentum and non-zero wavelength to prevent the inactivation of forceįield at absolute zero and singularity (infinite interacting energy) at To a superconductor, a superstar contains extreme force fields that have Large stars and for GRBs, and as an alternative to black hole and gravastar. ![]() Singularity-free superstar is proposed as a model for the collapse of
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