Choose the following Pauli matrix realization, with its spinor basis fixed for the later Dirac adjoint:
The Pauli matrix multiplication rule verifies
Extending linearly therefore gives a two-dimensional Lie algebra representation. For an irreducible representation, it suffices to rule out an invariant line. Any such line would have to be an eigenline of , whose two eigenvalues are distinct. Those two coordinate lines are interchanged by , so neither is invariant. There is no proper nonzero invariant subspace.
This is a spinorial representation rather than a single-valued two-dimensional representation of the identity component of the specified orthogonal group:
The mismatch explicitly exhibits the need for the spin double cover. It causes no obstruction to the requested infinitesimal construction.

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