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      Quasi-normal modes: the "electrons" of black holes as "gravitational atoms"? Implications for the black hole information puzzle

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          Abstract

          Some recent important results on black hole (BH) quantum physics concerning the BH effective state and the natural correspondence between Hawking radiation and BH quasi-normal modes (QNMs) are reviewed, clarified and refined. Such a correspondence permits to naturally interpret QNMs as quantum levels in a semi-classical model. This is a model of BH somewhat similar to the historical semi-classical model of the structure of a hydrogen atom introduced by Bohr in 1913. In a certain sense, QNMs represent the "electron" which jumps from a level to another one and the absolute values of the QNMs frequencies "triggered" by emissions (Hawking radiation) and absorption of particles represent the energy "shells" of the "gravitational hydrogen atom". Important consequences on the BH information puzzle are discussed. In fact, it is shown that the time evolution of this "Bohr-like BH model" obeys to a time dependent Schr\"odinger equation which permits the final BH state to be a pure quantum state instead of a mixed one. Thus, information comes out in BH evaporation, in agreement with the assumption by 't Hooft that Schr\"oedinger equations can be used universally for all dynamics in the universe. We also show that, in addition, our approach solves the entanglement problem connected with the information paradox. We emphasize that Bohr model is an approximated model of the hydrogen atom with respect to the valence shell atom model of full quantum mechanics. In the same way, we expect the Bohr-like BH model to be an approximated model with respect to the definitive, but at the present time unknown, BH model arising from a full quantum gravity theory.

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          Hawking Radiation as Tunneling

          We present a short and direct derivation of Hawking radiation as a tunneling process, based on particles in a dynamical geometry. The imaginary part of the action for the classically forbidden process is related to the Boltzmann factor for emission at the Hawking temperature. Because the derivation respects conservation laws, the exact spectrum is not precisely thermal. We compare and contrast the problem of spontaneous emission of charged particles from a charged conductor.
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            The quantum mass spectrum of the Kerr black hole

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              I.On the constitution of atoms and molecules

              N BOHR (1913)
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                Author and article information

                Journal
                2015-02-26
                2015-03-31
                Article
                10.1155/2015/867601
                1503.00565
                187429d7-b048-47af-a408-6a7d5c807adb

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
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                Adv. High En. Phys. 867601 (2015)
                31 pages, review paper. Invited contribution accepted for publication in the Advances in High Energy Physics Special Issue "Dark Atoms and Dark Radiation 2015", edited by Maxim Khlopov, Konstantin Belotsky, Jean-Ren\'e Cudell and Chris Kouvaris. Title changed with respect to the first version. The results of arXiv:1304.1899 and arXiv:1210.7747 has been carefully reviewed and refined
                gr-qc

                General relativity & Quantum cosmology
                General relativity & Quantum cosmology

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