Start from the three-index transformation law and contract the first two Cartesian indices:
Orthogonality supplies , where is the Kronecker delta. The remaining factor is exactly the vector transformation rule. Therefore is a vector.
This tensor contraction removes two indices by pairing them through the Euclidean metric. In general nonorthonormal coordinates, contraction must use the appropriate metric or pair a covariant and a contravariant index; the bare repeated-lower-index sum relies on Cartesian orthonormal coordinates.

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