We demonstrate that the very extended G+++ group element of the form gA=exp(−1(β,β)lnNβ⋅H)exp((1−N)Eβ)gA=exp(−(β,β)1lnNβ⋅H)exp((1−N)Eβ) describes the usual BPS, electric, single brane solutions found in G+++ theories.
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