摘要

In this paper, we derive the unitary transformation that relates the q (q) over bar chiral basis {R; I J(PC)} to the {I; (2S+1) L-J}-basis in a front-form framework. From the most general expression for the Clebsch-Gordan coefficients of the Poincare group one can see that the chiral limit brings the angular momentum coupling into a simple form that permits the relation in terms of SU(2) Clebsch-Gordan coefficients. We demonstrate that such a transformation is identical to the one obtained for canonical spin in the instant form.

  • 出版日期2012-11-10