Extends the equivalence of second-order EOM to first-order Bogomolnyi equations from single real/complex scalars to arbitrary real multi-component scalar fields without fixing the Lagrangian.
(35) As it can be seen this is the same result obtained in the previous section: R = ±1 then LXij φ′ j = Wφi
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Multi-component scalar fields and the complete factorization of its equations of motion
Extends the equivalence of second-order EOM to first-order Bogomolnyi equations from single real/complex scalars to arbitrary real multi-component scalar fields without fixing the Lagrangian.