For a Lie algebra representation , an invariant vector is a vector annihilated by every represented Lie algebra element:
The condition is zero infinitesimal action, not . The invariant vectors form a vector subspace.
For a one-dimensional abelian Lie algebra acting on through , the invariant vectors are exactly the first coordinate line. For the Adjoint representation, invariants are the center of a Lie algebra, because .
If the representation differentiates a representation of a connected Lie group, Lie algebra invariants are also group invariants. Connectedness matters: a disconnected group can act nontrivially even when its Lie algebra acts trivially. The sign action of has zero Lie algebra but no nonzero fixed vector.

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