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G+++ and Brane Solutions

Abstract

We demonstrate that the very extended G+++ group element of the form gA=exp⁑(βˆ’1(Ξ²,Ξ²)ln⁑NΞ²β‹…H)exp⁑((1βˆ’N)EΞ²)g_A=\exp(-{\frac{1}{(\beta,\beta)}\ln N}\beta \cdot H)\exp((1-N)E_\beta) describes the usual BPS, electric, single brane solutions found in G+++ theories.Comment: One new equation, added references, corrected typos and minor changes, 42 pages, 6 figures, LaTeX2

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