2020
DOI: 10.1103/physrevd.101.086019
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Brane universe and holography in the spacetime of a charged AdS dilaton black hole

Abstract: In the background of a charged AdS dilaton black hole, we investigate the movement of a selfgraviting 3-brane and relevant holographic effects as the brane move close to the AdS boundary. The induced metric on brane corresponds to an exact FLRW geometry, while the evolution of brane is determined by Israel junction condition and the effective Einstein field equation on brane together. When the brane approaches the AdS boundary, AdS/CFT correspondence implies that a radiation dominated FLRW-universe (P = 1 3 ρ)… Show more

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Cited by 2 publications
(6 citation statements)
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“…For getting a finite mass of black hole, we need to find a well-defined quasilocal stress-energy T tt . Thus, we choose the undetermined coefficients in (17) as [45]. After substitute these coefficients and ( 11)-( 15) into (22), the expression of black hole mass is obtained as…”
Section: Ads Dilaton Black Holes and Relevant Thermodynamical Quantitiesmentioning
confidence: 99%
See 4 more Smart Citations
“…For getting a finite mass of black hole, we need to find a well-defined quasilocal stress-energy T tt . Thus, we choose the undetermined coefficients in (17) as [45]. After substitute these coefficients and ( 11)-( 15) into (22), the expression of black hole mass is obtained as…”
Section: Ads Dilaton Black Holes and Relevant Thermodynamical Quantitiesmentioning
confidence: 99%
“…where we have used the (42). In brief, (45) means that the complexity growth rate, especially in the late time limit, can not exceed the bound 8πM √ 3 , whatever how large the dilaton coupling α is.…”
Section: The Growth Rate Of Complexity For Charged Ads-dilaton Black ...mentioning
confidence: 99%
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