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Black Objects and Hoop Conjecture in Five-dimensional Space-time

http://www.is.oit.ac.jp/~shinkai/

GR19 @ Mexico City, July 2010

Hisa-aki Shinkai

(Osaka Institute of Technology, Japan) work with Yuta Yamada (OIT)

Initial Data

Yamada & HS, CQG 27 (2010) 045012 Evolution

Yamada & HS, in preparation.

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1. Motivation and Goal

Higher-Dim Black Holes have

Rich

Structures

LHC experiments will (or will not) reveal Higher-Dim BHs in near future

4-dim BH : horizon is S^2, stable solutions

Schwarzschild --- Birkoff theorem (M)

Kerr --- uniqueness theorem (M, J)

Brane-World models give new viewpoints to gravity and cosmology

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4-dim BHs     Higher-dim BHs : Schwarzschild    Tangherlini

       --- unique & stable Kerr    Myers-Perry

       --- maybe unstable in higher J black ring (Emparan-Reall)

black Saturn

di-rings, orthogonal di-rings, ...

"Black Objects"

1. Motivation and Goal

Higher-Dim Black Holes have

Rich

Structures

(4)

4-dim BHs     Higher-dim BHs : Schwarzschild    Tangherlini

       --- unique & stable Kerr    Myers-Perry

       --- maybe unstable in higher J black ring (Emparan-Reall)

black Saturn

di-rings, orthogonal di-rings, ...

"Black Objects"

1. Motivation and Goal

Higher-Dim Black Holes have

Rich

Structures

(5)

black hole black string black ring

black Saturn

di-rings, orthogonal di-rings ...

"Black Objects"

Uniqueness (only in spherical sym.) Stability?

Formation Process?

Dynamical Features? ...

1. Motivation and Goal

Higher-Dim Black Holes have

Rich

Structures

(6)

black hole black string black ring

black Saturn

di-rings, orthogonal di-rings ...

"Black Objects"

Uniqueness (only in spherical sym.) Stability?

Formation Process?

Dynamical Features? ...

1. Motivation and Goal

Higher-Dim Black Holes have

Rich

Structures

No Hair Conjecture?

Cosmic Censorship?

Hoop Conjecture?

(7)

2. Initial Data Construction

- time symmetric, asymptotically flat - conformal flat

- non-rotating homogeneous dust

- in spheroidal shape or ring shape

- solve the Hamiltonian constraint eq. 512^2 grids - Apparent Horizon Search

both for Ring Horizon and Common Horizon - Define Hoop and check the Hoop Conjecture

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2.A: Initial Data Construction

metric & Hamiltonian constraint

Toroidal Cases

Spheroidal Cases

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Apparent Horizons Search

Toroidal Cases

Spheroidal Cases

Common Horizon

Ring Horizon

2.A: Initial Data Construction

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Area of Horizons

Toroidal Cases

Spheroidal Cases

Common Horizon

Ring Horizon

2.A: Initial Data Construction

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2.B: Initial Data Results

Spheroidal Cases

テキストテキストテキスト

cf. (3-dim.) Nakamura-Shapiro-Teukolsky (1988)

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2.B: Initial Data Results

Spheroidal Cases

テキストテキストテキスト

cf. (3-dim.) Nakamura-Shapiro-Teukolsky (1988)

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2.B: Initial Data Results

Toroidal Cases

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2.B: Initial Data Results

Toroidal Cases

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Hoop Conjecture

Hyper-Hoop conjecture ?

2.C. Initial Data Analysis

Hyper-Hoop Conjecture

Thorne (1972)

Penrose (1969) Ida-Nakao (2002)

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Hoop Conjecture

Hyper-Hoop conjecture ?

2.C. Initial Data Analysis

Hyper-Hoop Conjecture

Thorne (1972)

Penrose (1969) Ida-Nakao (2002)

In 5-D, if mass gets compacted

in some area, ....

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Spheroidal Cases

Hyper-Hoop conjecture ?

2.C. Initial Data Analysis

Define Hyper-Hoop as the surface

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Spheroidal Cases

Hyper-Hoop conjecture ?

2.C. Initial Data Analysis

Define Hyper-Hoop as the surface

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Spheroidal Cases

Hyper-Hoop conjecture ?

2.C. Initial Data Analysis

Define Hyper-Hoop as the surface

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Hyper-Hoop conjecture ? Toroidal Cases

2.C. Initial Data Analysis

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Hyper-Hoop conjecture ? Toroidal Cases

2.C. Initial Data Analysis

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Hyper-Hoop conjecture ? Toroidal Cases

2.C. Initial Data Analysis

Hyper-Hoop

does not work for

ring horizons.

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3. Evolution Code

- ADM full 4+1, ADM 2+1 Double Axisym Cartoon - 33^4 grids, 65^2 x 2^2 grids

- Maximal slicing condition, zero shift vectors - asymptically flat

- Collisionless Particles (5000) - the same total mass

- no rotation

- Apparent Horizon Search

both for Ring Horizon and Common Horizon

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3. Evolution (case I)

t=0 No Horizon

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3. Evolution (case I)

t=0 No Horizon

t=0.2 Common Horizon

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3. Evolution (case I)

t=0 No Horizon

t=0.2 Common Horizon

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3. Evolution (case I)

t=0 No Horizon

t=0.2 Common Horizon

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3. Evolution (case I)

t=0 No Horizon

t=0.2 Common Horizon

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t=0 No Horizon

3. Evolution (case II)

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t=0 No Horizon t=0.9 Ring Horizon

3. Evolution (case II)

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t=0 No Horizon t=0.9 Ring Horizon

3. Evolution (case II)

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t=0 No Horizon t=0.9 Ring Horizon

t=1.1 Common Horizon

3. Evolution (case II)

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t=0 No Horizon t=0.9 Ring Horizon

t=1.1 Common Horizon

3. Evolution (case II)

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t=0 No Horizon t=0.9 Ring Horizon

t=1.1 Common Horizon

3. Evolution (case II)

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t=0 No Horizon

3. Evolution (case III)

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t=0 No Horizon

t=1.19 Ring Horizon

3. Evolution (case III)

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t=0 No Horizon

t=1.19 Ring Horizon

3. Evolution (case III)

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t=0 No Horizon

t=1.19 Ring Horizon

3. Evolution (case III)

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t=0 No Horizon

t=1.19 Ring Horizon

3. Evolution (case III)

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t=0 No Horizon

t=1.19 Ring Horizon

3. Evolution (case III)

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t=0 No Horizon

t=1.19 Ring Horizon

3. Evolution (case III)

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4. Summary and Future Plans

Initial Data:

Topology of horizon changes with matter configurations Hyper-Hoop prediction

works well for formations of spheroidal black holes but not for rings.

Evolution:

no horizon    common horizon ring horizon

Future Plans:

include rotation, change slicing conditions search event horizon,

investigate the stability, formation/decay process,....

Towards Dynamics of 5-dim Black Objects

参照

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