Fractured Boer-Mulders effect in the production of polarized baryons

The fractured Boer-Mulders functions, Delta M-N(B up arrow/{q, q}up arrow:p)q(x; p(TN); z, (p) over right arrow (T).(k) over right arrow (T); Q(2)), describe an intriguing class of polarization effects for the production of baryons in the target fragmentation region of deep-inelastic processes. These functions characterize transverse momentum asymmetries related to the spin orientation for different flavors of axial-vector diquarks, {q(i), q(j)}up arrow, in an unpolarized ensemble of protons just as the familiar Boer-Mulders functions characterize transverse momentum asymmetries connected to the spin orientation of quarks in unpolarized targets. The asymmetries in p(TN) of the fractured Boer-Mulders effect originating in the proton distribution function can be separated kinematically, both in semi-inclusive deep-inelastic scattering and in the Drell-Yan process, from the asymmetries in k(TN) of the polarizing fracture functions, Delta M-N(B up arrow/{q, q}:p)q(x; p(T)(2); z, k(TN); Q(2)), generated during the soft color rearrangement of the fragmentation process. The experimental requirements for this separation are presented in this article and it is shown that the fractured Boer-Mulders effect should change sign between Drell-Yan and semi-inclusive deep-inelastic scattering while the polarizing fracture functions remain the same. Simple isospin arguments indicate the two polarization mechanisms should give significantly different results for the production of polarized Lambda's and Sigma's.