Let , since the original vectors form a basis. The reciprocal basis is
Taking the dot product with each gives , using orthogonality of a cross product and cyclic symmetry of the scalar triple product. If , taking its dot product with yields . The three reciprocal vectors are therefore linearly independent and form a basis of .
Equivalently, if has columns and columns , then , so . In particular any vector has coordinates , even when the original basis is not orthonormal.

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