Abstract

We demonstrate that the very extended G+++ group element of the form gA=exp⁡(−1(β,β)ln⁡Nβ⋅H)exp⁡((1−N)Eβ)g_A=\exp(-{\frac{1}{(β,β)}\ln N}β\cdot H)\exp((1-N)E_β) describes the usual BPS, electric, single brane solutions found in G+++ theories.

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