Differentiate the eigenvalue equation along the assumed smooth normalized eigenbranch:
Since is real symmetric, . Multiplying the differentiated equation by and using cancels the terms containing :
Thus the finite-dimensional Hellmann–Feynman theorem gives
Equivalently, differentiating the normalization gives and eliminates those terms from the derivative of . The proof needs the smooth eigenbranch assumed in the question; the smallest eigenvalue need not be differentiable at an arbitrary crossing without that assumption.

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