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SL(4,R) sigma model & Charged black rings

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Presentation on theme: "SL(4,R) sigma model & Charged black rings"— Presentation transcript:

1 SL(4,R) sigma model & Charged black rings
Da-Sheng Kung Chiang-Mei Chen National Central University, Taiwan 8 January 2008

2 Neutral black ring The black ring is a five-dimensional black hole with an event horizon of topology S1×S2

3 SL(4,R) σ-model The starting point is a five-dimensional action with gravity, dilaton field, and three-form field We perform a two-step reduction to three-dimensional theory in which all physical variables can be transformed to scalar fields

4 SL(4,R) σ-model The three-dimensional action is rewritten as
This action is invariant under the 15-parametric SL(4,R) transformations R-transformation: pure gauge. S-transformation: two gauge, three different scale, and two electric Harrison transformations. L-transformation: two magnetic Harrison transformations and Ehlers-like part of S-duality.

5 Asymptotic flatness preserving
The general SL(4,R) transformation can be represented by generator Define to be the asymptotic form of matrix Suppose it’s symmetric, then asymptotic flatness preserving requires that This will give the condition

6 Asymptotic flatness preserving
The flat geometry of black ring is The corresponding scalar potentials of target space are

7 Asymptotic flatness preserving
According to the asymptotic condition, only four transformations keep asymptotic flatness: Pure gauge: Electric Harrison: (generating Kaluza-Klein vector) Gauge & magnetic Harrison: (generating form field)

8 Charged black ring For constructing charged ring solution, it’s natural to choose neutral black ring as the seed solution where Define a useful function After reduction to three-dimensional theory, vector fields can be parameterized by

9 S3 transformation where
The electric charge is produced by the electric Harrison transformation with the parameter So that where

10 S3 transformation Black ring with Kaluza-Klein charge takes the form
The Kaluza-Klein vector is with components

11 R2+L3 transformation Since the transformed matrix then becomes

12 R2+L3 transformation By the relationship between matrix elements and target-space potentials, one can obtain where

13 R2+L3 transformation Black ring with form-field charge reads
The corresponding gauge potentials are

14 Thank You


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