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We expand the superpotential of $\nu$MSSM to 6th order. This is the order atwhich all flat directions can be lifted. All 5179 couplings are independent ie.the superpotential cannot be zero for all fields, without all couplings beingzero. Likewise, any gauge invariant potential to the 6th order can be made byfixing the constants. A specific and welldefined choice of normalisation hasbeen adopted. The case for investigating this potential, rather than looking atone or several generalised flat directions is made.

$\nu$MSSM superpotential to 6th order - normalised and with no superfluous couplings