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Charged black holes in string-inspired gravity models

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Presentation on theme: "Charged black holes in string-inspired gravity models"β€” Presentation transcript:

1 Charged black holes in string-inspired gravity models
Based on Hansen and DY, Hansen and DY, in preparation Leung Center for Cosmology and Particle Astrophysics, National Taiwan University Dong-han Yeom

2 Double-null formalism : brief review

3 Double-null formalism
Double-null formalism is a numerical procedure to solve Einstein equations. Using double-null metric ansatz, we overcome the coordinate singularity problem. Solve all equations: for example, for the simplest case, 3

4 Implementation Einstein tensors / energy-momentum tensors / scalar-field equation 4

5 Implementation Evolution equations - Einstein equations
- Field equation 5

6 Boundary condition We should give boundary conditions for all functions and their first derivatives at the initial in-going and out-going null lines. - (0,0) : From the Misner-Sharp mass function, by choosing the initial mass and radius 𝒓(𝟎,𝟎), we can determine 𝜢 𝟎,𝟎 , 𝒓 ,𝒖 (𝒖,𝟎), and 𝒓 ,𝒗 (𝟎,𝒗). - In-going null surface: First, we can choose matter sector 𝑺(𝒖,𝟎). Then, 𝑺 ,𝒖 (𝒖,𝟎) is already determined. From the Einstein equation of 𝒓 ,𝒖𝒖 part, we can obtain 𝜢 ,𝒖 (𝒖,𝟎). Then, we can obtain 𝜢 𝒖,𝟎 by integration. Second, we calculate the remained part from the equations of 𝒖𝒗 derivatives: 𝒓 ,𝒗 (𝒖,𝟎) from the equation for 𝒓 ,𝒖𝒗 , 𝜢 ,𝒗 (𝒖,𝟎) from the equation for 𝜢 ,𝒖𝒗 , and 𝑺 ,𝒗 (𝒖,𝟎) from the equation for 𝑺 ,𝒖𝒗 . - Out-going null surface: we can apply the same method. 6

7 Example: a neutral black hole in Einstein gravity
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8 Example: a neutral black hole in Einstein gravity
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9 Applications Double-null formalism can be extended to various ways.
Matter: neutral matter, gauge field, various potential and vacuum energy, … Gravity: Einstein gravity, dilaton gravity, Brans-Dicke gravity, f(R) gravity, … Dimensions: 4D, 3D, 4+nD, … Symmetries: spherical, hyperbolic, planar, circular, … 9

10 Charged black holes in string-inspired models

11 String-inspired models
We investigate the following model as a prototype of the sting-inspired models. 11

12 String-inspired models
We investigate the following model as a prototype of the sting-inspired models. There are some origins from string theory: Dilaton gravity 12

13 String-inspired models
We investigate the following model as a prototype of the sting-inspired models. There are some origins from string theory: Dilaton gravity Couplings to gauge sector 13

14 String-inspired models
We investigate the following model as a prototype of the sting-inspired models. There are some origins from string theory: Dilaton gravity Couplings to gauge sector Brane-world 14

15 String-inspired models
We investigate the following model as a prototype of the sting-inspired models. There are some origins from string theory: Dilaton gravity Couplings to gauge sector Brane-world Higher curvature corrections (e.g., f(R)) 15

16 String-inspired models
We implement the following model to double-null formalism. 16

17 Causal structures 17

18 Causal structures 18

19 Causal structures Except for the Type IIA inspired case, there is no Cauchy horizon and mass inflation inside a charged black hole. 19

20 Causal structures Except for the Type IIA inspired case, there is no Cauchy horizon and mass inflation inside a charged black hole. Is this a general nature of string theory? The answer is maybe NO. 20

21 Causal structures Except for the Type IIA inspired case, there is no Cauchy horizon and mass inflation inside a charged black hole. Is this a general nature of string theory? The answer is maybe NO. The key is in the dynamics of the Brans-Dicke field. 21

22 Responses of the Brans-Dicke sector
Responses of the Brans-Dicke field is determined by the following equation. 22

23 Responses of the Brans-Dicke sector
Responses of the Brans-Dicke field is determined by the following equation. 23

24 Responses of the Brans-Dicke sector
Responses of the Brans-Dicke field is determined by the following equation. If the dilaton field is β€˜stabilized’ by a potential term, then the equation should have one more term. 24

25 Return of mass inflation
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26 Return of mass inflation
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27 Conclusion We investigated (and are investigating) gravitational collapses of string-inspired models using double-null formalism. Especially, this is useful to investigate the fully dynamical process, e.g., internal structures of a charged black hole or a dynamical formation of the Brans-Dicke hair. As long as there is a Brans-Dicke hair, the internal structure has a space-like singularity without a Cauchy horizon. On the other hand, if the Brans-Dicke hair can be controlled by introducing a potential term, then the causal structure returns to mass inflation with a Cauchy horizion. A gravitational collapse can perturb a moduli field or a dilaton field; hence, a gravitational collapse can be a good window to see stringy effects. In addition, the observation of dilaton/moduli hair can teach us internal structure of a black hole (even though we do not fall into the black hole). 27

28 Thank you very much


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