2010
DOI: 10.1103/physrevd.81.124011
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Physics of the interior of a black hole with an exotic scalar matter

Abstract: We use a numerical code to consider the nonlinear processes arising when a Reissner-Nordstrom black hole is irradiated by an exotic scalar field (modelled as a free massless scalar field with an opposite sign for its energy-momentum tensor). These processes are quite different from the processes arising in the case of the same black hole being irradiated by a pulse of a normal scalar field. In our case, we did not observe the creation of a spacelike strong singularity in the T-region of the space-time. We inve… Show more

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Cited by 30 publications
(29 citation statements)
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“…In Ohm's words, this was attributed to the fact that "the '+' temperature possibilities of [the receiver temperature uncertainties] must predominate" [16]. Doroshkevich and Novikov cited Ohm's paper in a 1964 review of cosmic radiation predicted in Gamow's theory of the origin of the universe [17]. Perhaps due to a misinterpretation of the 3.3 K excess, Doroshkevich and Novikov attributed the excess temperature to emission from the Earth's atmosphere.…”
Section: Historical Motivationmentioning
confidence: 99%
“…In Ohm's words, this was attributed to the fact that "the '+' temperature possibilities of [the receiver temperature uncertainties] must predominate" [16]. Doroshkevich and Novikov cited Ohm's paper in a 1964 review of cosmic radiation predicted in Gamow's theory of the origin of the universe [17]. Perhaps due to a misinterpretation of the 3.3 K excess, Doroshkevich and Novikov attributed the excess temperature to emission from the Earth's atmosphere.…”
Section: Historical Motivationmentioning
confidence: 99%
“…To the best knowledge of the authors, the double-null formalism is one of the most efficient techniques to investigate the interior of the black holes [32] and we have priviously used this approach with good success [47-49, 57, 66]. There are some previous works regarding string-inspired models using the double-null formalism [33][34][35][36][37][38][39][40][41][42][43][44] and other methods [45,46] as well as the authors' previous works [47][48][49][50][51][52][53][54][55]. In this paper we will investigate a wide parameter space, for example, we will cover not only directly stringinspired models, but also indirectly string-inspired models (f (R) inspired model [56]) as well as natural generalizations of the parameters, e.g., the ghost limit.…”
Section: Jhep10(2014)040mentioning
confidence: 99%
“…where Equations (3.31) and (3.39) are evolution equations for α ,uv , r ,uv , Φ ,uv and s ,uv , which can be solved with the same integration scheme used in the authors' previous papers [47][48][49]57]. The gauge field a can be evolved using the same numerical scheme via Equation (3.38) or we can evolve a and q via Equations (3.34) and (3.35).…”
Section: Jhep10(2014)040mentioning
confidence: 99%
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“…Therefore, much attention is given to this question in the literature (see [1][2][3][4][5][6][7][8][9]). The simplest wormhole model [10][11][12] (a phantom scalar field with a negative kinetic term) turned out to be unstable, contrary to the erroneous assertions in [1,2] and in accordance with the more recent (indepen dent) correct studies [3][4][5][6][7]13]). The more complex model of the same wormhole with the same metric [6,7] (a radial magnetic field and phantom dust with a negative mass density) turned out to be almost stable against all spherical perturbation modes (except the longitudinal radial dust motion by inertia).…”
Section: Introductionmentioning
confidence: 99%