- #1
Zeev Vager
What are the references (published journals) for the following:
Unfortunately this argument is not true since the weak-interaction current is precisely of (V-A) form, i.e., you subtract the axial-vector from the vector current. Of course, your argument is true, when considering only parity-conserving interactions (strong, electromagnetic). Further, in relativistic quantum mechanics there is no unique frame-independent splitting of orbital angular momentum and spin. Thus it is not easy to answer the question within relativistic theory, but of course total angular momentum must be an axial vector.
Unfortunately this argument is not true since the weak-interaction current is precisely of (V-A) form, i.e., you subtract the axial-vector from the vector current. Of course, your argument is true, when considering only parity-conserving interactions (strong, electromagnetic). Further, in relativistic quantum mechanics there is no unique frame-independent splitting of orbital angular momentum and spin. Thus it is not easy to answer the question within relativistic theory, but of course total angular momentum must be an axial vector.