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On Black String/Brane Instability and its Fate

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On Black String/Brane Instability and its Fate. Gungwon Kang at KISTI ... F. Pretorius; www.tapir.caltech.edu/~fransp/ Garfinkle, Lehner & Pretorius: '04 ... – PowerPoint PPT presentation

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Title: On Black String/Brane Instability and its Fate


1
On Black String/Brane Instability and its Fate
Mar. 22, 2006 at the NR Spring School
  • Gungwon Kang at KISTI

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

3
I. 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?

5
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6
  • Gravitational perturbations 93 GL

Lichnerowicz Eq.
Massive spin-2 fields!
7
0
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!?

10
  • Horowitz Maeda (01)

The bs horizon cannot pinch off in a finite time,
but becomes a non-uniform one as a final state.
11
Issues
  • 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

12
II. 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

14
For s-wave fluctuations
15
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16
Results 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!
18
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19
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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

21
Perturbed horizon in the case of ?_4 0 with a
3-brane 00 Gregory
22
  • Black branes in D 4
  • BTZ black string 05 GK Y. Lee in preparation

23
NO 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

25
III. Fate of the GL instability
  • Horowitz-Maeda conjecture

gt 0 (Area theorem)
26
Thus,
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.

28
F. 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.
30
IV. 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?

32
Potential for the mode solutions in the
z-direction
Effective box potential!
33
  • BTZ black string in 4D
  • - Stable always!
  • - No matter field!

34
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35
Accommodation at Daejeon
  • Matt and his family ? Spapia hotel
  • D. Choi, Martin, and others
  • ? KAIST Intl Village A

KAIST
KISTI
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