We investigate the geometric content of the first-order part of the Laplace–Beltrami operator on an oriented Riemannian manifold. Relative to an arbitrary local orthonormal frame, the first-order part of the Laplace–Beltrami operator defines a distinguished vector field, whose coefficients are expressed through the Levi–Civita connection forms. The corresponding one-form determines a covariant derivative whose connection factorization removes the first-order part of the Laplace–Beltrami operator and replaces it by a natural scalar potential. The construction is frame dependent. We show that its transformation under local rotations of the orthonormal frame compensates the corresponding variation of the sum-of-squares part, leaving the full Laplace–Beltrami operator invariant. These results reveal the geometric role of the first-order part of the Laplace–Beltrami operator.

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