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Volumn 77, Issue 2, 2008, Pages

Gravitational dynamics in s+1+1 dimensions II. Hamiltonian theory

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EID: 38049162136     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.77.024003     Document Type: Article
Times cited : (33)

References (14)
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    • Gergely1    Á, L.2
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  • 13
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    • Note that in Eq. (32) there is a Lie-derivative with respect to ∂/∂ χ instead of ∂/∂t. In the second Eq. 47 of this paper M should be replaced by N, in Eqs. 62 63 64 65 κ∼2Λ∼ by Λ∼, the right-hand side of Eqs. 64 65 should contain additional κ∼2 factors, and the formulas 53 55 63 65 only hold for s=3, the first two of them being given correctly as Eqs. 6 8 of the present paper. Equations (D3)-(D4c) have to be replaced by Eqs. 1 2 of the present paper. The isotropic pressure p is denoted as P in the present paper.
    • Note that in Eq. (32) there is a Lie-derivative with respect to ∂/∂ χ instead of ∂/∂t. In the second Eq. 47 of this paper M should be replaced by N, in Eqs. 62 63 64 65 κ∼2Λ∼ by Λ∼, the right-hand side of Eqs. 64 65 should contain additional κ∼2 factors, and the formulas 53 55 63 65 only hold for s=3, the first two of them being given correctly as Eqs. 6 8 of the present paper. Equations (D3)-(D4c) have to be replaced by Eqs. 1 2 of the present paper. The isotropic pressure p is denoted as P in the present paper.


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