Project the first-order equation onto , with . By orthonormality and the Hermitian operator property,
Consequently
and
The numerator order is important: the question defines with on the bra, whereas projecting the correction onto state gives . The two coincide only when the relevant matrix element is real.
Excluding an component chooses , a permitted first-order phase and wavefunction normalization convention. A component parallel to is not determined by the projected equation. Nondegeneracy ensures nonzero denominators; a small energy gap can still make the perturbative expansion inaccurate unless .

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