For , directly contract the supplied vector:
Thus whenever its stated normalization is defined, namely and . This is the Pauli-Lubanski orthogonality property.
The description as a unit vector, however, needs an additional assumption. From the given components and the mass shell,
It equals minus one only for spin parallel to momentum, including the zero-momentum case. A concrete counterexample is and : the proposed normalized vector has square minus two. Orthogonality is still true. A genuine Pauli-Lubanski pseudovector constructed by boosting a fixed rest-frame spin has invariant norm ; the source's generic spatial expression and denominator do not supply that normalization for arbitrary .

Articles by others on the same topic (0)

There are currently no matching articles.