Title: On Black String/Brane Instability and its Fate
1On Black String/Brane Instability and its Fate
Mar. 22, 2006 at the NR Spring School
2- Introduction
- Black string or brane solutions
- Stability
- Fate of the GL instability
- II. Stability of various black branes
- Various black Dp-branes
- Black strings in AdS space
- Black branes in D 4
- Higher order gravity theories
- III. Fate of the GL instability
- Horowitz-Maeda conjecture
- Numerical evolution
- IV. Research plan
3I. Introduction
- Black string or brane solutions
x(t,r,?,f)
z
Ex)
4 Stability?
- Schwarzschild black holes in any dimensions
- STABLE under linearized perturbations
- This property seems to hold for any stationary
- black hole having spherical event horizon.
- What about for black strings/branes?
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6- Gravitational perturbations 93 GL
Lichnerowicz Eq.
Massive spin-2 fields!
70
8- Fate of the GL instability?
- Black string fragmentation
- The GL instability and this fragmentation
scenario are used in various discussions such as - black holes in M theory, various unstable
D-brane configurations, etc. - black holes in brane world models
- instability of rapidly rotating black holes in
higher dimensions (D gt 5) - instability of black rings in D5
9- If the black string horizon pinches off, a naked
singularity may occur. - Violation of the cosmic censorship conjecture!?
- For the case of charged black strings,
- Violation of the charge conservation!?
10The bs horizon cannot pinch off in a finite time,
but becomes a non-uniform one as a final state.
11Issues
- How robust is the GL instability?
- ? Stability in a wider class of black
string/brane backgrounds, in a different
dynamics, etc. - Any confirmation for the final fate of the GL
instability? - ? Full nonlinear evolution numerically,
perturbative analyses in higher order - Any sort of uniqueness theorem for black
string/brane configuration? - ? Studies on solution space
12II. Stability of various black branes
- Basic features of the GL instability
- If L , no instability.
- The extremal black string should be stable.
- Strong curvature on the horizon probably gives
strong GL instability. - Non-uniformity may give stabilization effect.
13- Charged black Dp-branes in type II supergravity
- 03 Hirayama, GK Y. Lee
14For s-wave fluctuations
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16Results for some interesting objects
- All extremal black branes are
- STABLE (BPS states)
- Magnetically charged black NS5, D5,D6 branes
- UNSTABLE ALWAYS
17- Black strings in AdS space 01 Hirayama GK
Not uniform, but warped!
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20- Thus,
- dS_4/M_4-Schwarzschild black strings
- UNSTABLE ALWAYS
- But,
- AdS_4-Schwarzschild black string
- STABLE if r_ gt
21Perturbed horizon in the case of ?_4 0 with a
3-brane 00 Gregory
22- BTZ black string 05 GK Y. Lee in preparation
23NO UNSTABLE MODE SOLUTION!
24- Higher order gravity theories
- Motivations
- - String theory
- - Relevant for strong gravity region
- e.g., pinching off of a black string
- Work in progress D. Park, M. Park GK
25III. Fate of the GL instability
- Horowitz-Maeda conjecture
gt 0 (Area theorem)
26Thus,
The sphere cannot shrink to zero size in finite
affine time. A non-uniform bs would be the
end-state of the GL instability.
27- Numerical simulations for a neutral black
string 03 Choptuik et al.
28F. Pretorius www.tapir.caltech.edu/fransp/
29- Garfinkle, Lehner Pretorius 04
It might be true that the neutral BS pinches off
in an infinite affine time.
30IV. Research plan
- The issue about the end-state of the GL
instability has not been resolved yet. - All numerical results for full evolutions so far
are based on the studies only for neutral black
strings. - We have seen that charged black strings, black
strings in AdS space, and BTZ black strings
behave differently under small perturbations. - ? Expect that numerical studies for these black
string spacetimes may give some hints at
understanding the end-state of the GL instability!
31- Propose investigations on the full numerical
evolution of these types of perturbed black
strings near the critical point
- Charged black branes in supergravity
- - Very interesting, but probably not easy due
to - the gauge field!
- AdS_4-Schwarzschild black string in 5D
- - Fairly easy due to the absence of matter
field! - - Exists some reason for expecting quick
- stabilization! gt 1st example confirming
HMs?
32Potential for the mode solutions in the
z-direction
Effective box potential!
33- BTZ black string in 4D
- - Stable always!
- - No matter field!
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35Accommodation at Daejeon
- Matt and his family ? Spapia hotel
- D. Choi, Martin, and others
-
- ? KAIST Intl Village A
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